Leveraging genomic signatures of oral microbiome-associated antibiotic resistance genes for diagnosing pancreatic cancer

Growing evidence has increasingly suggested a potential linkage between the oral microbiome and various diseases, including pancreatic ductal adenocarcinoma (PDAC). However, the utilization of gene-level information derived from the oral microbiome for diagnosing PDAC remains unexplored. In this study, we sought to investigate the novel potential of leveraging genomic signatures associated with antibiotic resistance genes (ARGs) within the oral microbiome for the diagnosis of PDAC. By conducting an analysis of oral microbiome samples obtained from PDAC patients, we successfully identified specific ARGs that displayed distinct sequence abundance profiles correlated with the presence of PDAC. In the healthy group, three ARGs were found to be enriched, whereas 21 ARGs were enriched in PDAC patients. Remarkably, these ARGs from oral microbiome exhibited promising diagnostic capabilities for PDAC (AUROC = 0.79), providing a non-invasive and early detection method. Our findings not only provide novel modal data for diagnosing PDAC but also shed light on the intricate interplay between the oral microbiome and PDAC.

Enhancing Built-in Electric Fields via Molecular Symmetry Modulation in Supramolecular Photocatalysts for Highly Efficient Photocatalytic Hydrogen Evolution

Nature-inspired supramolecular self-assemblies are attractive photocatalysts, but their quantum yields are limited by poor charge separation and transportation. A promising strategy for efficient charge transfer is to enhance the built-in electric field by symmetry breaking. Herein, an unsymmetric protonation, N-heterocyclic π-conjugated anthrazoline-based supramolecular photocatalyst SA-DADK-H+ was developed. The unsymmetric protonation breaks the initial structural symmetry of DADK, resulting in ca. 50-fold increase in the molecular dipole, and facilitates efficient charge separation and transfer within SA-DADK-H+. The protonation process also creates numerous active sites for H2O adsorption, and serves as crucial proton relays, significantly improving the photocatalytic efficiency. Remarkably, SA-DADK-H+ exhibits an outstanding hydrogen evolution rate of 278.2 mmol g-1 h-1 and a remarkable apparent quantum efficiency of 25.1% at 450 nm, placing it among the state-of-the-art performances in organic semiconductor photocatalysts. Furthermore, the versatility of the unsymmetric protonation approach has been successfully applied to four other photocatalysts, enhancing their photocatalytic performance by 39 to 533 times. These findings highlight the considerable potential of unsymmetric protonation induced symmetry breaking strategy in tailoring supramolecular photocatalysts for efficient solar-to-fuel production.

Establishment and evaluation of rat models of parastomal hernia

PURPOSE

Parastomal hernia poses a challenging problem in the field of hernia surgery. The high incidence and recurrence rates of parastomal hernia necessitate surgeons to enhance surgical techniques and repair materials. This study aimed to develop a rat model of parastomal hernia by inducing various types of defects on the abdominal wall with colostomy. This established method has potential for future studies on parastomal hernia.

METHODS

In this study, 32 male rats were included and randomly divided into four groups: the oblique abdominis excision (OE), oblique abdominis dissection (OD), rectus abdominis excision (RE), and rectus abdominis dissection (RD) groups. In each group, colostomy was performed and an abdominal wall defect was induced. The rats were observed for 28 days following surgery. The survival rate, body weight, parastomal hernia model scores, abdominal wall adhesion and inflammation, and collagen level in the hernial sac were compared.

RESULTS

No significant differences in survival rate and weight were observed among the four groups. The parastomal hernia model scores in the RE and RD groups were significantly higher than those in the OE and OD groups. The ratio of collagen I/III in the RE and RD groups was significantly lower than that in the OE and OD groups. Adhesion and inflammation levels were lower in the RE group than in the RD group.

CONCLUSION

Based on a comprehensive comparison of the findings, RE with colostomy emerged as the optimal approach for establishing parastomal hernia models in rats.

Isobavachalcone induces hepatotoxicity in zebrafish embryos and HepG2 cells via the System Xc--GSH-GPX4 signaling pathway in ferroptosis response

Isobavachalcone (IBC) is a flavonoid component of the traditional Chinese medicine Psoraleae Fructus, with a range of pharmacological properties. However, IBC causes some hepatotoxicity, and the mechanism of toxicity is unclear. The purpose of this paper was to investigate the possible mechanism of toxicity of IBC on HepG2 cells and zebrafish embryos. The results showed that exposure to IBC increased zebrafish embryo mortality and decreased hatchability. Meanwhile, IBC induced liver injury and increased expression of ALT and AST activity. Further studies showed that IBC caused the increase of ROS and MDA the decrease of CAT, GSH, and GSH-Px; the increase of Fe2+ content; and the changes of ferroptosis related genes (acsl4, gpx4, and xct) and iron storage related genes (tf, fth, and fpn) in zebrafish embryos. Through in vitro verification, it was found that IBC also caused oxidative stress and increased Fe2+ content in HepG2 cells. IBC caused depolarization of mitochondrial membrane potential (MMP) and reduction of mitochondrial ATP, as well as altered expression of ACSl4, SLC7A11, GPX4, and FTH1 proteins. Treatment of HepG2 cells with ferrostatin-1 could reverse the effect of IBC. Targeting the System Xc--GSH-GPX4 pathway of ferroptosis and preventing oxidative stress damage might offer a theoretical foundation for practical therapy and prevention of IBC-induced hepatotoxicity.

Ferrous gluconate triggers ferroptosis in Escherichia coli: Implications of lipid peroxidation and DNA damage

Microbial ferroptosis has been proved to combat drug-resistant pathogens, but whether this pattern can be applied to the prevention and control of Escherichia coli remains to be further explored. In this study, ferrous gluconate (FeGlu) showed remarkable efficacy in killing E. coli MG1655 with a mortality rate exceeding 99.9%, as well as enterotoxigenic E. coli H10407 (ETEC H10407) and enterohemorrhagic E. coli O157:H7 (EHEC O157:H7). Bacteria death was instigated by the infiltration of Fe2+, accompanied by a burst of intracellular reactive oxygen species (ROS) and lipid peroxidation. Notably, mitigating lipid peroxidation failed to alleviate death of E. coli. Further findings confirmed that FeGlu induced DNA damage, and ΔrecA mutant showed more sensitive, implicating that DNA damage was involved in the death of E. coli. The direct interaction of Fe2+ with DNA was demonstrated by fluorescent staining, gel electrophoresis, and circular dichroism (CD). Moreover, proteomic analysis unveiled 50 differentially expressed proteins (DEPs), including 18 significantly down-regulated proteins and 32 significantly up-regulated proteins. Among them, the down-regulation of SOS-responsive transcriptional suppressor LexA indicated DNA damage induced severely by FeGlu. Furthermore, FeGlu influenced pathways such as fatty acid metabolism (FadB, FadE), iron-sulfur cluster assembly (IscA, IscU, YadR), iron binding, and DNA-binding transcription, along with α-linolenic acid metabolism, fatty acid degradation, and pyruvate metabolism. These pathways were related to FeGlu stress, including lipid peroxidation and DNA damage. In summary, FeGlu facilitated ferroptosis in E. coli through mechanisms involving lipid peroxidation and DNA damage, which presents a new strategy for the development of innovative antimicrobial strategies targeting E. coli infections.

Amplitude Analysis of the B^{0}→K^{*0}μ^{+}μ^{-} Decay

An amplitude analysis of the B^{0}→K^{*0}μ^{+}μ^{-} decay is presented using a dataset corresponding to an integrated luminosity of 4.7  fb^{-1} of pp collision data collected with the LHCb experiment. For the first time, the coefficients associated to short-distance physics effects, sensitive to processes beyond the standard model, are extracted directly from the data through a q^{2}-unbinned amplitude analysis, where q^{2} is the μ^{+}μ^{-} invariant mass squared. Long-distance contributions, which originate from nonfactorizable QCD processes, are systematically investigated, and the most accurate assessment to date of their impact on the physical observables is obtained. The pattern of measured corrections to the short-distance couplings is found to be consistent with previous analyses of b- to s-quark transitions, with the largest discrepancy from the standard model predictions found to be at the level of 1.8 standard deviations. The global significance of the observed differences in the decay is 1.4 standard deviations.

Mechanism of action of microRNA166 on nitric oxide in alfalfa (Medicago sativa L.) under drought stress

BACKGROUND

Alfalfa is a perennial forage crop of high importance, but its cultivation is often affected by drought stress. Currently, the investigation of drought-related small RNAs is a popular research topic to uncover plant drought resistance mechanisms. Among these small RNAs, microRNA166 (miR166) is associated with drought in numerous plant species. Initial small RNA sequencing studies have shown that miR166 is highly responsive to exogenous nitric oxide (NO) and drought. Therefore, analyzing the expression of Msa-miR166 under nitric oxide and drought treatment is significant.

RESULT

Bioinformatics analysis revealed that the miR166 family is widely distributed among plants, ranging from mosses to eudicots, with significant distribution differences between species. The evolutionary degree of Msa-miR166s is highly similar to that of Barrel medic (Medicago truncatula) and Soybean (Glycine max), but significantly different from the model plant Arabidopsis (Arabidopsis thaliana). It is suggested that there are no significant differences in miR166s within the species, and members of Msa-miR166s can form a typical stem-loop. The lowest level of exogenous nitric oxide was observed in Msa-miR166s under drought stress, followed by individual drought, and the highest level was observed after removing endogenous nitric oxide.

CONCLUSION

In response to short-term drought, Msa-miR166s down-regulate expression in alfalfa (Medicago sativa L.). Exogenous nitric oxide can reduce the expression of Msa-miR166s in response to short-term drought. These findings suggest that Msa-miR166e-5p is responsive to environmental changes. The expression levels of target genes showed an opposite trend to Msa-miR166s, verifying the accuracy of Degradome sequencing in the early stage. This suggests that alfalfa experiences drought stress when regulated by exogenous nitric oxide, targeting HD ZIP-III, FRI, and CoA ligase genes. Additionally, the expression of Msa-miR166s in response to drought stress varies between leaves and roots, indicating spatiotemporal specificity.

Mechanism of Nicotiflorin in San-Ye-Qing rhizome for anti-inflammatory effect in ulcerative colitis

BACKGROUND

The incidence of ulcerative colitis (UC) is on the rise globally and the development of drugs targeting UC is urgent. Finding the target of action of natural products is important for drug discovery, elucidation of drug action mechanism, and disease mechanism. San-Ye-Qing (SYQ), is an ancient herbal medicine, but whether the powder of its rhizome has pharmacological effects against UC and its mechanism of action are not clear.

PURPOSE

To evaluate the therapeutic effectiveness of rhizome powder of SYQ in treating UC, and conduct an isolation and characterization of the chemical constituents of the powder. Further, screen the most potent compounds among them and determine the potential mechanism for treating UC.

METHODS

In vivo, the therapeutic effect of SYQ's rhizome powder on UC was assessed by mice's body weight, DAI score, colon length, tissue MPO activity, serum inflammatory markers, etc. Additionally, HPLC was used to isolate and identify the specific chemical components of SYQ's rhizome powder. Then, the most effective compounds and their therapeutic targets were analysed and screened in SYQ rhizome powder using network pharmacology, combined with CCK-8 assay, NO release assay and molecular docking assay, in conjunction with CETSA, DARTS, SPR and enzyme activity assay. Finally, the biological effects of the key compound on the targets were validated using Western blot and ELISA.

RESULTS

In vivo, SYQ rhizome powder effectively restored mice's body weight, lowered DAI and pathological score, downregulated the expression of inflammatory biomarkers, and restored colon length, as well as the colonic epithelial and mucus barriers. Afterward, 9 compounds were isolated and identified from the powder of the rhizomes of SYQ by HPLC. Nicotiflorin is the primary compound in SYQ with the highest concentration. According to both CCK-8 and NO release tests, Nicotiflorin is also the most efficacious compound. Combined with network pharmacological prediction, molecular docking analysis, CETSA, DARTS, SPR and enzyme activity assay, Nicotiflorin may ultimately suppress inflammation by targeting p65 and inhibiting the NF-κB pathway, thereby attenuating the activation of NLRP3 inflammasome. To verify this conclusion, Western blot and ELISA experiments were conducted.

CONCLUSIONS

Our results suggest that the extract from SYQ rhizomes has therapeutic properties for UC. Its active ingredient Nicotiflorin exerted potent anti-UC effects by binding to p65 and inhibiting the activation of NF-κB and NLRP3 inflammasomes.

Feasibility of stereotactic optical navigation for needle positioning in percutaneous nephrolithotomy

BACKGROUND

This study assessed the feasibility of acquiring single-attempt access to the pelvicalyceal system during percutaneous nephrolithotomy (PCNL) using stereotactic optical navigation combined with cone-beam CT (CBCT) imaging.

METHODS

Patients with a PCNL indication were prospectively included in this IRB approved study. After sterile preparation, fiducial markers were attached to patients' skin. An initial intraprocedural CBCT scan was acquired, on which the urologist planned the needle trajectory using the navigation software. After verifying that no critical structures were crossed, the needle guide was aligned with the plan. A needle was manually inserted through the needle guide to the indicated depth and a second CBCT scan was performed for needle position confirmation. Both, scanning and needle insertion, were performed under apnea. The study evaluated technical success, accuracy, procedure time, complication rate, and radiation dose.

RESULTS

Between June 2022 and April 2023, seven patients were included. In all patients, the navigation system allowed safe puncture. However, the technical success rate was only 29%. In 42% of the cases, pelvicalyceal access was achieved by a small manual adjustment. In the remaining 29%, the needle was retracted and positioned per clinical standard. The average deviation between the needle and target was 5.9 ± 2.3 mm. The average total procedure time was 211 ± 44 min. The average radiation exposure was 6.4 mSv, with CBCT scanning contributing to 82% of this exposure.

CONCLUSIONS

The optical navigation system facilitated safe needle insertion but did not consistently ensure accurate one-attempt needle positioning for PCNL. Real-time visualization and trajectory correction may improve the technical success rate.

Reliability of Droplet Digital PCR Alone and in Combination with Interleukin-6 and Procalcitonin for Prognosis of Bloodstream Infection

Purpose

Bloodstream infection(BSI) is linked with high mortality, underscoring the significance of prompt etiological diagnosis for timely and precise treatment. This study aims to investigate the diagnostic value of droplet digital polymerase chain reaction(ddPCR) in combination with conventional inflammatory markers [interleukin-6(IL-6) and procalcitonin(PCT)] concerning disease progression and treatment prognosis in BSI patients. Furthermore, the study aims to explore a more efficient clinical application strategy.

Patients and Methods

This prospective case seried study centers on 176 patients suspected of or confirmed with BSI. Blood samples were collected to extract nucleic acids for identifying pathogens (bacteria, fungi, and viruses) and determining copy loads via ddPCR.

Results

The sensitivity of ddPCR was markedly higher compared to the culture method (74.71% vs 31.03%). A positive correlation existed between bacterial load and levels of inflammatory markers [IL-6 (P=0.0182), PCT (P=0.0029), and CRP (P=0.0005)]. In suspected BSI cases, the combination of ddPCR and inflammatory markers could predict sepsis risk [ROC: Area under the curve(AUC)=0.6071, P=0.0383]. Within confirmed BSI patients, the ddPCR bacterial load of those with SOFA<7 was lower than that of the SOFA≥7 (P=0.0334). ddPCR (OR: 1.789, P=0.035) monitoring combined with PCT (OR: 1.787, P=0.035) holded predictive value for SOFA progression (AUC=0.7913, P=0.0003). Similarly, BSI survivors displayed a lower burden than non-survivors (P=0.0170). Additionally, ddPCR combinated with IL-6 provided a more accurate and expedited insight into clinical outcomes prediction for BSI confirmed patients (AUC=0.7352, P=0.0030). Serial monitoring of bacterial load by ddPCR effectively mirrored the clinical course of BSI in patients. Notably, patients with positive ddPCR virus infection exhibited significantly reduced lymphocyte counts (P=0.0003).

Conclusion

In a clinical context, qualitative ddPCR results and quantitative continuous monitoring can more precisely assess sepsis progression and treatment prognosis in BSI patients. Furthermore, ddPCR results offer quicker and more accurate reference points for clinical antibacterial and antiviral interventions.

[ANCA-negative granulomatosis with polyangiitis: a case report]

We reported a case of 73-year-old male with multiple pulmonary nodules and cavities. The patient was admitted with a chief complaint of "dry cough with shortness of breath for 3 months". Chest CT showed multiple irregular masses, nodules, and patchy lesions in both lungs, accompanied by the formation of cavities. He also had anemia and renal dysfunction. Despite given empirical anti-infective and anti-tuberculosis treatments, the pulmonary nodules progressed, and the cavities enlarged. Anti-neutrophil cytoplasmic antibodies (ANCA) were negative twice. Bronchoscopic biopsy was performed. The mucosal pathology of the right middle lobe lesion showed little necrosis, focal granulomatous structure formation, and relevant vasculitis and remaining vessel wall structure in the necrosis lesions by elastic fiber staining. A clinical diagnosis of ANCA-negative necrotizing granulomatous polyangiitis was made and the patient was treated with glucocorticoids and cyclophosphamide. The nodules and cavities shrank, and some lesions were absorbed.

Fraction of χ_{c} Decays in Prompt J/ψ Production Measured in pPb Collisions at sqrt[s_{NN}]=8.16 TeV

The fraction of χ_{c1} and χ_{c2} decays in the prompt J/ψ yield, F_{χ_{c}→J/ψ}=σ_{χ_{c}→J/ψ}/σ_{J/ψ}, is measured by the LHCb detector in pPb collisions at sqrt[s_{NN}]=8.16  TeV. The study covers the forward (1.5 Collapse

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Affiliation(s)

R Aaij Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands
A S W Abdelmotteleb Department of Physics, University of Warwick, Coventry, United Kingdom
C Abellan Beteta Physik-Institut, Universität Zürich, Zürich, Switzerland
F Abudinén Department of Physics, University of Warwick, Coventry, United Kingdom
T Ackernley Oliver Lodge Laboratory, University of Liverpool, Liverpool, United Kingdom
B Adeva Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
M Adinolfi H.H. Wills Physics Laboratory, University of Bristol, Bristol, United Kingdom
P Adlarson Department of Physics and Astronomy, Uppsala University, Uppsala, Sweden (associated with School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom)
C Agapopoulou European Organization for Nuclear Research (CERN), Geneva, Switzerland
C A Aidala University of Michigan, Ann Arbor, Michigan, USA (associated with Syracuse University, Syracuse, New York, USA)
Z Ajaltouni Université Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France
S Akar University of Cincinnati, Cincinnati, Ohio, USA
K Akiba Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands
P Albicocco INFN Laboratori Nazionali di Frascati, Frascati, Italy
J Albrecht Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
F Alessio European Organization for Nuclear Research (CERN), Geneva, Switzerland
M Alexander School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom
A Alfonso Albero ICCUB, Universitat de Barcelona, Barcelona, Spain
Z Aliouche Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
P Alvarez Cartelle Cavendish Laboratory, University of Cambridge, Cambridge, United Kingdom
R Amalric LPNHE, Sorbonne Université, Paris Diderot Sorbonne Paris Cité, CNRS/IN2P3, Paris, France
S Amato Universidade Federal do Rio de Janeiro (UFRJ), Rio de Janeiro, Brazil
J L Amey H.H. Wills Physics Laboratory, University of Bristol, Bristol, United Kingdom
Y Amhis Université Paris-Saclay, CNRS/IN2P3, IJCLab, Orsay, France European Organization for Nuclear Research (CERN), Geneva, Switzerland
L An School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China
L Anderlini INFN Sezione di Firenze, Firenze, Italy
M Andersson Physik-Institut, Universität Zürich, Zürich, Switzerland
A Andreianov Affiliated with an institute covered by a cooperation agreement with CERN
P Andreola Physik-Institut, Universität Zürich, Zürich, Switzerland
M Andreotti INFN Sezione di Ferrara, Ferrara, Italy
D Andreou Syracuse University, Syracuse, New York, USA
A A Anelli INFN Sezione di Milano-Bicocca, Milano, Italy
D Ao University of Chinese Academy of Sciences, Beijing, China
F Archilli INFN Sezione di Roma Tor Vergata, Roma, Italy
M Argenton INFN Sezione di Ferrara, Ferrara, Italy
S Arguedas Cuendis Consejo Nacional de Rectores (CONARE), San Jose, Costa Rica
A Artamonov Affiliated with an institute covered by a cooperation agreement with CERN
M Artuso Syracuse University, Syracuse, New York, USA
E Aslanides Aix Marseille Univ, CNRS/IN2P3, CPPM, Marseille, France
M Atzeni Massachusetts Institute of Technology, Cambridge, Massachusetts, USA
B Audurier Laboratoire Leprince-Ringuet, CNRS/IN2P3, Ecole Polytechnique, Institut Polytechnique de Paris, Palaiseau, France
D Bacher Department of Physics, University of Oxford, Oxford, United Kingdom
I Bachiller Perea Université Savoie Mont Blanc, CNRS, IN2P3-LAPP, Annecy, France
S Bachmann Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
M Bachmayer Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
J J Back Department of Physics, University of Warwick, Coventry, United Kingdom
A Bailly-Reyre LPNHE, Sorbonne Université, Paris Diderot Sorbonne Paris Cité, CNRS/IN2P3, Paris, France
P Baladron Rodriguez Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
V Balagura Laboratoire Leprince-Ringuet, CNRS/IN2P3, Ecole Polytechnique, Institut Polytechnique de Paris, Palaiseau, France
W Baldini INFN Sezione di Ferrara, Ferrara, Italy
J Baptista de Souza Leite Centro Brasileiro de Pesquisas Físicas (CBPF), Rio de Janeiro, Brazil
M Barbetti INFN Sezione di Firenze, Firenze, Italy
I R Barbosa Pontifícia Universidade Católica do Rio de Janeiro (PUC-Rio), Rio de Janeiro, Brazil (associated with Universidade Federal do Rio de Janeiro (UFRJ), Rio de Janeiro, Brazil)
R J Barlow Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
S Barsuk Université Paris-Saclay, CNRS/IN2P3, IJCLab, Orsay, France
W Barter School of Physics and Astronomy, University of Edinburgh, Edinburgh, United Kingdom
M Bartolini Cavendish Laboratory, University of Cambridge, Cambridge, United Kingdom
F Baryshnikov Affiliated with an institute covered by a cooperation agreement with CERN
J M Basels I. Physikalisches Institut, RWTH Aachen University, Aachen, Germany
G Bassi INFN Sezione di Pisa, Pisa, Italy
B Batsukh Institute Of High Energy Physics (IHEP), Beijing, China
A Battig Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
A Bay Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
A Beck Department of Physics, University of Warwick, Coventry, United Kingdom
M Becker Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
F Bedeschi INFN Sezione di Pisa, Pisa, Italy
I B Bediaga Centro Brasileiro de Pesquisas Físicas (CBPF), Rio de Janeiro, Brazil
A Beiter Syracuse University, Syracuse, New York, USA
S Belin Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
V Bellee Physik-Institut, Universität Zürich, Zürich, Switzerland
K Belous Affiliated with an institute covered by a cooperation agreement with CERN
I Belov INFN Sezione di Genova, Genova, Italy
I Belyaev Affiliated with an institute covered by a cooperation agreement with CERN
G Benane Aix Marseille Univ, CNRS/IN2P3, CPPM, Marseille, France
G Bencivenni INFN Laboratori Nazionali di Frascati, Frascati, Italy
E Ben-Haim LPNHE, Sorbonne Université, Paris Diderot Sorbonne Paris Cité, CNRS/IN2P3, Paris, France
A Berezhnoy Affiliated with an institute covered by a cooperation agreement with CERN
R Bernet Physik-Institut, Universität Zürich, Zürich, Switzerland
S Bernet Andres DS4DS, La Salle, Universitat Ramon Llull, Barcelona, Spain
H C Bernstein Syracuse University, Syracuse, New York, USA
C Bertella Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
A Bertolin Università degli Studi di Padova, Università e INFN, Padova, Padova, Italy
C Betancourt Physik-Institut, Universität Zürich, Zürich, Switzerland
F Betti School of Physics and Astronomy, University of Edinburgh, Edinburgh, United Kingdom
J Bex Cavendish Laboratory, University of Cambridge, Cambridge, United Kingdom
Ia Bezshyiko Physik-Institut, Universität Zürich, Zürich, Switzerland
J Bhom Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland
M S Bieker Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
N V Biesuz INFN Sezione di Ferrara, Ferrara, Italy
P Billoir LPNHE, Sorbonne Université, Paris Diderot Sorbonne Paris Cité, CNRS/IN2P3, Paris, France
A Biolchini Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands
M Birch Imperial College London, London, United Kingdom
F C R Bishop Université Savoie Mont Blanc, CNRS, IN2P3-LAPP, Annecy, France
A Bitadze Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
A Bizzeti School of Physics and Astronomy, Monash University, Melbourne, Australia Centro Brasileiro de Pesquisas Físicas (CBPF), Rio de Janeiro, Brazil Universidade Federal do Rio de Janeiro (UFRJ), Rio de Janeiro, Brazil Center for High Energy Physics, Tsinghua University, Beijing, China Institute Of High Energy Physics (IHEP), Beijing, China School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China University of Chinese Academy of Sciences, Beijing, China Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China Consejo Nacional de Rectores (CONARE), San Jose, Costa Rica Université Savoie Mont Blanc, CNRS, IN2P3-LAPP, Annecy, France Université Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France Aix Marseille Univ, CNRS/IN2P3, CPPM, Marseille, France Université Paris-Saclay, CNRS/IN2P3, IJCLab, Orsay, France Laboratoire Leprince-Ringuet, CNRS/IN2P3, Ecole Polytechnique, Institut Polytechnique de Paris, Palaiseau, France LPNHE, Sorbonne Université, Paris Diderot Sorbonne Paris Cité, CNRS/IN2P3, Paris, France I. Physikalisches Institut, RWTH Aachen University, Aachen, Germany Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany Max-Planck-Institut für Kernphysik (MPIK), Heidelberg, Germany Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany School of Physics, University College Dublin, Dublin, Ireland INFN Sezione di Bari, Bari, Italy INFN Sezione di Bologna, Bologna, Italy INFN Sezione di Ferrara, Ferrara, Italy INFN Sezione di Firenze, Firenze, Italy INFN Laboratori Nazionali di Frascati, Frascati, Italy INFN Sezione di Genova, Genova, Italy INFN Sezione di Milano, Milano, Italy INFN Sezione di Milano-Bicocca, Milano, Italy INFN Sezione di Cagliari, Monserrato, Italy Università degli Studi di Padova, Università e INFN, Padova, Padova, Italy INFN Sezione di Perugia, Perugia, Italy INFN Sezione di Pisa, Pisa, Italy INFN Sezione di Roma La Sapienza, Roma, Italy INFN Sezione di Roma Tor Vergata, Roma, Italy Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands Nikhef National Institute for Subatomic Physics and VU University Amsterdam, Amsterdam, Netherlands AGH - University of Science and Technology, Faculty of Physics and Applied Computer Science, Kraków, Poland Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland National Center for Nuclear Research (NCBJ), Warsaw, Poland Horia Hulubei National Institute of Physics and Nuclear Engineering, Bucharest-Magurele, Romania Affiliated with an institute covered by a cooperation agreement with CERN DS4DS, La Salle, Universitat Ramon Llull, Barcelona, Spain ICCUB, Universitat de Barcelona, Barcelona, Spain Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain Instituto de Fisica Corpuscular, Centro Mixto Universidad de Valencia - CSIC, Valencia, Spain European Organization for Nuclear Research (CERN), Geneva, Switzerland Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland Physik-Institut, Universität Zürich, Zürich, Switzerland NSC Kharkiv Institute of Physics and Technology (NSC KIPT), Kharkiv, Ukraine Institute for Nuclear Research of the National Academy of Sciences (KINR), Kyiv, Ukraine University of Birmingham, Birmingham, United Kingdom H.H. Wills Physics Laboratory, University of Bristol, Bristol, United Kingdom Cavendish Laboratory, University of Cambridge, Cambridge, United Kingdom Department of Physics, University of Warwick, Coventry, United Kingdom STFC Rutherford Appleton Laboratory, Didcot, United Kingdom School of Physics and Astronomy, University of Edinburgh, Edinburgh, United Kingdom School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom Oliver Lodge Laboratory, University of Liverpool, Liverpool, United Kingdom Imperial College London, London, United Kingdom Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom Department of Physics, University of Oxford, Oxford, United Kingdom Massachusetts Institute of Technology, Cambridge, Massachusetts, USA University of Cincinnati, Cincinnati, Ohio, USA University of Maryland, College Park, Maryland, USA Los Alamos National Laboratory (LANL), Los Alamos, New Mexico, USA Syracuse University, Syracuse, New York, USA Pontifícia Universidade Católica do Rio de Janeiro (PUC-Rio), Rio de Janeiro, Brazil (associated with Universidade Federal do Rio de Janeiro (UFRJ), Rio de Janeiro, Brazil) School of Physics and Electronics, Hunan University, Changsha City, China (associated with Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China) Guangdong Provincial Key Laboratory of Nuclear Science, Guangdong-Hong Kong Joint Laboratory of Quantum Matter, Institute of Quantum Matter, South China Normal University, Guangzhou, China (associated with Center for High Energy Physics, Tsinghua University, Beijing, China) Lanzhou University, Lanzhou, China (associated with Institute Of High Energy Physics (IHEP), Beijing, China) School of Physics and Technology, Wuhan University, Wuhan, China (associated with Center for High Energy Physics, Tsinghua University, Beijing, China) Departamento de Fisica, Universidad Nacional de Colombia, Bogota, Colombia (associated with LPNHE, Sorbonne Université, Paris Diderot Sorbonne Paris Cité, CNRS/IN2P3, Paris, France) Universität Bonn - Helmholtz-Institut für Strahlen und Kernphysik, Bonn, Germany (associated with Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany) Eotvos Lorand University, Budapest, Hungary (associated with European Organization for Nuclear Research (CERN), Geneva, Switzerland) Van Swinderen Institute, University of Groningen, Groningen, Netherlands (associated with Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands) Universiteit Maastricht, Maastricht, Netherlands (associated with Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands) Tadeusz Kosciuszko Cracow University of Technology, Cracow, Poland (associated with Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland) Department of Physics and Astronomy, Uppsala University, Uppsala, Sweden (associated with School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom) University of Michigan, Ann Arbor, Michigan, USA (associated with Syracuse University, Syracuse, New York, USA) Departement de Physique Nucleaire (SPhN), Gif-Sur-Yvette, France
M P Blago Cavendish Laboratory, University of Cambridge, Cambridge, United Kingdom
T Blake Department of Physics, University of Warwick, Coventry, United Kingdom
F Blanc Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
J E Blank Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
S Blusk Syracuse University, Syracuse, New York, USA
D Bobulska School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom
V Bocharnikov Affiliated with an institute covered by a cooperation agreement with CERN
J A Boelhauve Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
O Boente Garcia Laboratoire Leprince-Ringuet, CNRS/IN2P3, Ecole Polytechnique, Institut Polytechnique de Paris, Palaiseau, France
T Boettcher University of Cincinnati, Cincinnati, Ohio, USA
A Bohare School of Physics and Astronomy, University of Edinburgh, Edinburgh, United Kingdom
A Boldyrev Affiliated with an institute covered by a cooperation agreement with CERN
C S Bolognani Universiteit Maastricht, Maastricht, Netherlands (associated with Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands)
R Bolzonella INFN Sezione di Ferrara, Ferrara, Italy
N Bondar Affiliated with an institute covered by a cooperation agreement with CERN
F Borgato Università degli Studi di Padova, Università e INFN, Padova, Padova, Italy European Organization for Nuclear Research (CERN), Geneva, Switzerland
S Borghi Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
M Borsato INFN Sezione di Milano-Bicocca, Milano, Italy
J T Borsuk Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland
S A Bouchiba Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
T J V Bowcock Oliver Lodge Laboratory, University of Liverpool, Liverpool, United Kingdom
A Boyer European Organization for Nuclear Research (CERN), Geneva, Switzerland
C Bozzi INFN Sezione di Ferrara, Ferrara, Italy
M J Bradley Imperial College London, London, United Kingdom
S Braun University of Maryland, College Park, Maryland, USA
A Brea Rodriguez Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
N Breer Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
J Brodzicka Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland
A Brossa Gonzalo Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
J Brown Oliver Lodge Laboratory, University of Liverpool, Liverpool, United Kingdom
D Brundu INFN Sezione di Cagliari, Monserrato, Italy
A Buonaura Physik-Institut, Universität Zürich, Zürich, Switzerland
L Buonincontri Università degli Studi di Padova, Università e INFN, Padova, Padova, Italy
A T Burke Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
C Burr European Organization for Nuclear Research (CERN), Geneva, Switzerland
A Bursche Guangdong Provincial Key Laboratory of Nuclear Science, Guangdong-Hong Kong Joint Laboratory of Quantum Matter, Institute of Quantum Matter, South China Normal University, Guangzhou, China (associated with Center for High Energy Physics, Tsinghua University, Beijing, China)
A Butkevich Affiliated with an institute covered by a cooperation agreement with CERN
J S Butter Cavendish Laboratory, University of Cambridge, Cambridge, United Kingdom
J Buytaert European Organization for Nuclear Research (CERN), Geneva, Switzerland
W Byczynski European Organization for Nuclear Research (CERN), Geneva, Switzerland
S Cadeddu INFN Sezione di Cagliari, Monserrato, Italy
H Cai School of Physics and Technology, Wuhan University, Wuhan, China (associated with Center for High Energy Physics, Tsinghua University, Beijing, China)
R Calabrese INFN Sezione di Ferrara, Ferrara, Italy
L Calefice Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
S Cali INFN Laboratori Nazionali di Frascati, Frascati, Italy
M Calvi INFN Sezione di Milano-Bicocca, Milano, Italy
M Calvo Gomez DS4DS, La Salle, Universitat Ramon Llull, Barcelona, Spain
J Cambon Bouzas Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
P Campana INFN Laboratori Nazionali di Frascati, Frascati, Italy
D H Campora Perez Universiteit Maastricht, Maastricht, Netherlands (associated with Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands)
A F Campoverde Quezada University of Chinese Academy of Sciences, Beijing, China
S Capelli INFN Sezione di Milano-Bicocca, Milano, Italy
L Capriotti INFN Sezione di Ferrara, Ferrara, Italy
R Caravaca-Mora Consejo Nacional de Rectores (CONARE), San Jose, Costa Rica
A Carbone INFN Sezione di Bologna, Bologna, Italy
L Carcedo Salgado Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
R Cardinale INFN Sezione di Genova, Genova, Italy
A Cardini INFN Sezione di Cagliari, Monserrato, Italy
P Carniti INFN Sezione di Milano-Bicocca, Milano, Italy
L Carus Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
A Casais Vidal Massachusetts Institute of Technology, Cambridge, Massachusetts, USA
R Caspary Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
G Casse Oliver Lodge Laboratory, University of Liverpool, Liverpool, United Kingdom
J Castro Godinez Consejo Nacional de Rectores (CONARE), San Jose, Costa Rica
M Cattaneo European Organization for Nuclear Research (CERN), Geneva, Switzerland
G Cavallero INFN Sezione di Ferrara, Ferrara, Italy
V Cavallini INFN Sezione di Ferrara, Ferrara, Italy
S Celani Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
J Cerasoli Aix Marseille Univ, CNRS/IN2P3, CPPM, Marseille, France
D Cervenkov Department of Physics, University of Oxford, Oxford, United Kingdom
S Cesare INFN Sezione di Milano, Milano, Italy
A J Chadwick Oliver Lodge Laboratory, University of Liverpool, Liverpool, United Kingdom
I Chahrour University of Michigan, Ann Arbor, Michigan, USA (associated with Syracuse University, Syracuse, New York, USA)
M Charles LPNHE, Sorbonne Université, Paris Diderot Sorbonne Paris Cité, CNRS/IN2P3, Paris, France
Ph Charpentier European Organization for Nuclear Research (CERN), Geneva, Switzerland
C A Chavez Barajas Oliver Lodge Laboratory, University of Liverpool, Liverpool, United Kingdom
M Chefdeville Université Savoie Mont Blanc, CNRS, IN2P3-LAPP, Annecy, France
C Chen Aix Marseille Univ, CNRS/IN2P3, CPPM, Marseille, France
S Chen Institute Of High Energy Physics (IHEP), Beijing, China
A Chernov Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland
S Chernyshenko Institute for Nuclear Research of the National Academy of Sciences (KINR), Kyiv, Ukraine
V Chobanova Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
S Cholak Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
M Chrzaszcz Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland
A Chubykin Affiliated with an institute covered by a cooperation agreement with CERN
V Chulikov Affiliated with an institute covered by a cooperation agreement with CERN
P Ciambrone INFN Laboratori Nazionali di Frascati, Frascati, Italy
M F Cicala Department of Physics, University of Warwick, Coventry, United Kingdom
X Cid Vidal Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
G Ciezarek European Organization for Nuclear Research (CERN), Geneva, Switzerland
P Cifra European Organization for Nuclear Research (CERN), Geneva, Switzerland
P E L Clarke School of Physics and Astronomy, University of Edinburgh, Edinburgh, United Kingdom
M Clemencic European Organization for Nuclear Research (CERN), Geneva, Switzerland
H V Cliff Cavendish Laboratory, University of Cambridge, Cambridge, United Kingdom
J Closier European Organization for Nuclear Research (CERN), Geneva, Switzerland
J L Cobbledick Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
C Cocha Toapaxi Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
V Coco European Organization for Nuclear Research (CERN), Geneva, Switzerland
J Cogan Aix Marseille Univ, CNRS/IN2P3, CPPM, Marseille, France
E Cogneras Université Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France
L Cojocariu Horia Hulubei National Institute of Physics and Nuclear Engineering, Bucharest-Magurele, Romania
P Collins European Organization for Nuclear Research (CERN), Geneva, Switzerland
T Colombo European Organization for Nuclear Research (CERN), Geneva, Switzerland
A Comerma-Montells ICCUB, Universitat de Barcelona, Barcelona, Spain
L Congedo INFN Sezione di Bari, Bari, Italy
A Contu INFN Sezione di Cagliari, Monserrato, Italy
N Cooke School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom
I Corredoira Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
A Correia LPNHE, Sorbonne Université, Paris Diderot Sorbonne Paris Cité, CNRS/IN2P3, Paris, France
G Corti European Organization for Nuclear Research (CERN), Geneva, Switzerland
J J Cottee Meldrum H.H. Wills Physics Laboratory, University of Bristol, Bristol, United Kingdom
B Couturier European Organization for Nuclear Research (CERN), Geneva, Switzerland
D C Craik Physik-Institut, Universität Zürich, Zürich, Switzerland
M Cruz Torres Centro Brasileiro de Pesquisas Físicas (CBPF), Rio de Janeiro, Brazil
R Currie School of Physics and Astronomy, University of Edinburgh, Edinburgh, United Kingdom
C L Da Silva Los Alamos National Laboratory (LANL), Los Alamos, New Mexico, USA
S Dadabaev Affiliated with an institute covered by a cooperation agreement with CERN
L Dai School of Physics and Electronics, Hunan University, Changsha City, China (associated with Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China)
X Dai School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China
E Dall'Occo Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
J Dalseno Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
C D'Ambrosio European Organization for Nuclear Research (CERN), Geneva, Switzerland
J Daniel Université Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France
A Danilina Affiliated with an institute covered by a cooperation agreement with CERN
P d'Argent INFN Sezione di Bari, Bari, Italy
A Davidson Department of Physics, University of Warwick, Coventry, United Kingdom
J E Davies Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
A Davis Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
O De Aguiar Francisco Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
C De Angelis INFN Sezione di Cagliari, Monserrato, Italy
J de Boer Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands
K De Bruyn Van Swinderen Institute, University of Groningen, Groningen, Netherlands (associated with Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands)
S De Capua Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
M De Cian Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany European Organization for Nuclear Research (CERN), Geneva, Switzerland
U De Freitas Carneiro Da Graca Centro Brasileiro de Pesquisas Físicas (CBPF), Rio de Janeiro, Brazil
E De Lucia INFN Laboratori Nazionali di Frascati, Frascati, Italy
J M De Miranda Centro Brasileiro de Pesquisas Físicas (CBPF), Rio de Janeiro, Brazil
L De Paula Universidade Federal do Rio de Janeiro (UFRJ), Rio de Janeiro, Brazil
M De Serio INFN Sezione di Bari, Bari, Italy
D De Simone Physik-Institut, Universität Zürich, Zürich, Switzerland
P De Simone INFN Laboratori Nazionali di Frascati, Frascati, Italy
F De Vellis Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
J A de Vries Universiteit Maastricht, Maastricht, Netherlands (associated with Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands)
F Debernardis INFN Sezione di Bari, Bari, Italy
D Decamp Université Savoie Mont Blanc, CNRS, IN2P3-LAPP, Annecy, France
V Dedu Aix Marseille Univ, CNRS/IN2P3, CPPM, Marseille, France
L Del Buono LPNHE, Sorbonne Université, Paris Diderot Sorbonne Paris Cité, CNRS/IN2P3, Paris, France
B Delaney Massachusetts Institute of Technology, Cambridge, Massachusetts, USA
H-P Dembinski Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
J Deng Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China
V Denysenko Physik-Institut, Universität Zürich, Zürich, Switzerland
O Deschamps Université Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France
F Dettori INFN Sezione di Cagliari, Monserrato, Italy
B Dey Eotvos Lorand University, Budapest, Hungary (associated with European Organization for Nuclear Research (CERN), Geneva, Switzerland)
P Di Nezza INFN Laboratori Nazionali di Frascati, Frascati, Italy
I Diachkov Affiliated with an institute covered by a cooperation agreement with CERN
S Didenko Affiliated with an institute covered by a cooperation agreement with CERN
S Ding Syracuse University, Syracuse, New York, USA
V Dobishuk Institute for Nuclear Research of the National Academy of Sciences (KINR), Kyiv, Ukraine
A D Docheva School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom
A Dolmatov Affiliated with an institute covered by a cooperation agreement with CERN
C Dong Center for High Energy Physics, Tsinghua University, Beijing, China
A M Donohoe School of Physics, University College Dublin, Dublin, Ireland
F Dordei INFN Sezione di Cagliari, Monserrato, Italy
A C Dos Reis Centro Brasileiro de Pesquisas Físicas (CBPF), Rio de Janeiro, Brazil
L Douglas School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom
A G Downes Université Savoie Mont Blanc, CNRS, IN2P3-LAPP, Annecy, France
W Duan Guangdong Provincial Key Laboratory of Nuclear Science, Guangdong-Hong Kong Joint Laboratory of Quantum Matter, Institute of Quantum Matter, South China Normal University, Guangzhou, China (associated with Center for High Energy Physics, Tsinghua University, Beijing, China)
P Duda Tadeusz Kosciuszko Cracow University of Technology, Cracow, Poland (associated with Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland)
M W Dudek Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland
L Dufour European Organization for Nuclear Research (CERN), Geneva, Switzerland
V Duk INFN Sezione di Perugia, Perugia, Italy
P Durante European Organization for Nuclear Research (CERN), Geneva, Switzerland
M M Duras Tadeusz Kosciuszko Cracow University of Technology, Cracow, Poland (associated with Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland)
J M Durham Los Alamos National Laboratory (LANL), Los Alamos, New Mexico, USA
A Dziurda Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland
A Dzyuba Affiliated with an institute covered by a cooperation agreement with CERN
S Easo European Organization for Nuclear Research (CERN), Geneva, Switzerland STFC Rutherford Appleton Laboratory, Didcot, United Kingdom
E Eckstein Universität Bonn - Helmholtz-Institut für Strahlen und Kernphysik, Bonn, Germany (associated with Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany)
U Egede School of Physics and Astronomy, Monash University, Melbourne, Australia
A Egorychev Affiliated with an institute covered by a cooperation agreement with CERN
V Egorychev Affiliated with an institute covered by a cooperation agreement with CERN
C Eirea Orro Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
S Eisenhardt School of Physics and Astronomy, University of Edinburgh, Edinburgh, United Kingdom
E Ejopu Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
S Ek-In Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
L Eklund Department of Physics and Astronomy, Uppsala University, Uppsala, Sweden (associated with School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom)
M Elashri University of Cincinnati, Cincinnati, Ohio, USA
J Ellbracht Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
S Ely Imperial College London, London, United Kingdom
A Ene Horia Hulubei National Institute of Physics and Nuclear Engineering, Bucharest-Magurele, Romania
E Epple University of Cincinnati, Cincinnati, Ohio, USA
S Escher I. Physikalisches Institut, RWTH Aachen University, Aachen, Germany
J Eschle Physik-Institut, Universität Zürich, Zürich, Switzerland
S Esen Physik-Institut, Universität Zürich, Zürich, Switzerland
T Evans Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
F Fabiano INFN Sezione di Cagliari, Monserrato, Italy European Organization for Nuclear Research (CERN), Geneva, Switzerland
L N Falcao Centro Brasileiro de Pesquisas Físicas (CBPF), Rio de Janeiro, Brazil
Y Fan University of Chinese Academy of Sciences, Beijing, China
B Fang Université Paris-Saclay, CNRS/IN2P3, IJCLab, Orsay, France School of Physics and Technology, Wuhan University, Wuhan, China (associated with Center for High Energy Physics, Tsinghua University, Beijing, China)
L Fantini INFN Sezione di Perugia, Perugia, Italy
M Faria Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
K Farmer School of Physics and Astronomy, University of Edinburgh, Edinburgh, United Kingdom
D Fazzini INFN Sezione di Milano-Bicocca, Milano, Italy
L Felkowski Tadeusz Kosciuszko Cracow University of Technology, Cracow, Poland (associated with Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland)
M Feng Institute Of High Energy Physics (IHEP), Beijing, China University of Chinese Academy of Sciences, Beijing, China
M Feo European Organization for Nuclear Research (CERN), Geneva, Switzerland
M Fernandez Gomez Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
A D Fernez University of Maryland, College Park, Maryland, USA
F Ferrari INFN Sezione di Bologna, Bologna, Italy
F Ferreira Rodrigues Universidade Federal do Rio de Janeiro (UFRJ), Rio de Janeiro, Brazil
S Ferreres Sole Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands
M Ferrillo Physik-Institut, Universität Zürich, Zürich, Switzerland
M Ferro-Luzzi European Organization for Nuclear Research (CERN), Geneva, Switzerland
S Filippov Affiliated with an institute covered by a cooperation agreement with CERN
R A Fini INFN Sezione di Bari, Bari, Italy
M Fiorini INFN Sezione di Ferrara, Ferrara, Italy
M Firlej AGH - University of Science and Technology, Faculty of Physics and Applied Computer Science, Kraków, Poland
K M Fischer Department of Physics, University of Oxford, Oxford, United Kingdom
D S Fitzgerald University of Michigan, Ann Arbor, Michigan, USA (associated with Syracuse University, Syracuse, New York, USA)
C Fitzpatrick Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
T Fiutowski AGH - University of Science and Technology, Faculty of Physics and Applied Computer Science, Kraków, Poland
F Fleuret Laboratoire Leprince-Ringuet, CNRS/IN2P3, Ecole Polytechnique, Institut Polytechnique de Paris, Palaiseau, France
M Fontana INFN Sezione di Bologna, Bologna, Italy
F Fontanelli INFN Sezione di Genova, Genova, Italy
L F Foreman Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
R Forty European Organization for Nuclear Research (CERN), Geneva, Switzerland
D Foulds-Holt Cavendish Laboratory, University of Cambridge, Cambridge, United Kingdom
M Franco Sevilla University of Maryland, College Park, Maryland, USA
M Frank European Organization for Nuclear Research (CERN), Geneva, Switzerland
E Franzoso INFN Sezione di Ferrara, Ferrara, Italy
G Frau Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
C Frei European Organization for Nuclear Research (CERN), Geneva, Switzerland
D A Friday Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
L Frontini INFN Sezione di Milano, Milano, Italy
J Fu University of Chinese Academy of Sciences, Beijing, China
Q Fuehring Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
Y Fujii School of Physics and Astronomy, Monash University, Melbourne, Australia
T Fulghesu LPNHE, Sorbonne Université, Paris Diderot Sorbonne Paris Cité, CNRS/IN2P3, Paris, France
E Gabriel Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands
G Galati INFN Sezione di Bari, Bari, Italy
M D Galati Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands
A Gallas Torreira Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
D Galli INFN Sezione di Bologna, Bologna, Italy
S Gambetta European Organization for Nuclear Research (CERN), Geneva, Switzerland School of Physics and Astronomy, University of Edinburgh, Edinburgh, United Kingdom
M Gandelman Universidade Federal do Rio de Janeiro (UFRJ), Rio de Janeiro, Brazil
P Gandini INFN Sezione di Milano, Milano, Italy
H Gao University of Chinese Academy of Sciences, Beijing, China
R Gao Department of Physics, University of Oxford, Oxford, United Kingdom
Y Gao Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China
Y Gao School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China
Y Gao Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China
M Garau INFN Sezione di Cagliari, Monserrato, Italy
L M Garcia Martin Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
P Garcia Moreno ICCUB, Universitat de Barcelona, Barcelona, Spain
J García Pardiñas European Organization for Nuclear Research (CERN), Geneva, Switzerland
B Garcia Plana Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
K G Garg Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China
L Garrido ICCUB, Universitat de Barcelona, Barcelona, Spain
C Gaspar European Organization for Nuclear Research (CERN), Geneva, Switzerland
R E Geertsema Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands
L L Gerken Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
E Gersabeck Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
M Gersabeck Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
T Gershon Department of Physics, University of Warwick, Coventry, United Kingdom
Z Ghorbanimoghaddam H.H. Wills Physics Laboratory, University of Bristol, Bristol, United Kingdom
L Giambastiani Università degli Studi di Padova, Università e INFN, Padova, Padova, Italy
F I Giasemis LPNHE, Sorbonne Université, Paris Diderot Sorbonne Paris Cité, CNRS/IN2P3, Paris, France
V Gibson Cavendish Laboratory, University of Cambridge, Cambridge, United Kingdom
H K Giemza National Center for Nuclear Research (NCBJ), Warsaw, Poland
A L Gilman Department of Physics, University of Oxford, Oxford, United Kingdom
M Giovannetti INFN Laboratori Nazionali di Frascati, Frascati, Italy
A Gioventù ICCUB, Universitat de Barcelona, Barcelona, Spain
P Gironella Gironell ICCUB, Universitat de Barcelona, Barcelona, Spain
C Giugliano INFN Sezione di Ferrara, Ferrara, Italy
M A Giza Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland
E L Gkougkousis Imperial College London, London, United Kingdom
F C Glaser Université Paris-Saclay, CNRS/IN2P3, IJCLab, Orsay, France Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
V V Gligorov LPNHE, Sorbonne Université, Paris Diderot Sorbonne Paris Cité, CNRS/IN2P3, Paris, France
C Göbel Pontifícia Universidade Católica do Rio de Janeiro (PUC-Rio), Rio de Janeiro, Brazil (associated with Universidade Federal do Rio de Janeiro (UFRJ), Rio de Janeiro, Brazil)
E Golobardes DS4DS, La Salle, Universitat Ramon Llull, Barcelona, Spain
D Golubkov Affiliated with an institute covered by a cooperation agreement with CERN
A Golutvin Affiliated with an institute covered by a cooperation agreement with CERN European Organization for Nuclear Research (CERN), Geneva, Switzerland Imperial College London, London, United Kingdom
A Gomes Centro Brasileiro de Pesquisas Físicas (CBPF), Rio de Janeiro, Brazil
S Gomez Fernandez ICCUB, Universitat de Barcelona, Barcelona, Spain
F Goncalves Abrantes Department of Physics, University of Oxford, Oxford, United Kingdom
M Goncerz Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland
G Gong Center for High Energy Physics, Tsinghua University, Beijing, China
J A Gooding Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
I V Gorelov Affiliated with an institute covered by a cooperation agreement with CERN
C Gotti INFN Sezione di Milano-Bicocca, Milano, Italy
J P Grabowski Universität Bonn - Helmholtz-Institut für Strahlen und Kernphysik, Bonn, Germany (associated with Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany)
L A Granado Cardoso European Organization for Nuclear Research (CERN), Geneva, Switzerland
E Graugés ICCUB, Universitat de Barcelona, Barcelona, Spain
E Graverini Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
L Grazette Department of Physics, University of Warwick, Coventry, United Kingdom
G Graziani School of Physics and Astronomy, Monash University, Melbourne, Australia Centro Brasileiro de Pesquisas Físicas (CBPF), Rio de Janeiro, Brazil Universidade Federal do Rio de Janeiro (UFRJ), Rio de Janeiro, Brazil Center for High Energy Physics, Tsinghua University, Beijing, China Institute Of High Energy Physics (IHEP), Beijing, China School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China University of Chinese Academy of Sciences, Beijing, China Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China Consejo Nacional de Rectores (CONARE), San Jose, Costa Rica Université Savoie Mont Blanc, CNRS, IN2P3-LAPP, Annecy, France Université Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France Aix Marseille Univ, CNRS/IN2P3, CPPM, Marseille, France Université Paris-Saclay, CNRS/IN2P3, IJCLab, Orsay, France Laboratoire Leprince-Ringuet, CNRS/IN2P3, Ecole Polytechnique, Institut Polytechnique de Paris, Palaiseau, France LPNHE, Sorbonne Université, Paris Diderot Sorbonne Paris Cité, CNRS/IN2P3, Paris, France I. Physikalisches Institut, RWTH Aachen University, Aachen, Germany Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany Max-Planck-Institut für Kernphysik (MPIK), Heidelberg, Germany Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany School of Physics, University College Dublin, Dublin, Ireland INFN Sezione di Bari, Bari, Italy INFN Sezione di Bologna, Bologna, Italy INFN Sezione di Ferrara, Ferrara, Italy INFN Sezione di Firenze, Firenze, Italy INFN Laboratori Nazionali di Frascati, Frascati, Italy INFN Sezione di Genova, Genova, Italy INFN Sezione di Milano, Milano, Italy INFN Sezione di Milano-Bicocca, Milano, Italy INFN Sezione di Cagliari, Monserrato, Italy Università degli Studi di Padova, Università e INFN, Padova, Padova, Italy INFN Sezione di Perugia, Perugia, Italy INFN Sezione di Pisa, Pisa, Italy INFN Sezione di Roma La Sapienza, Roma, Italy INFN Sezione di Roma Tor Vergata, Roma, Italy Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands Nikhef National Institute for Subatomic Physics and VU University Amsterdam, Amsterdam, Netherlands AGH - University of Science and Technology, Faculty of Physics and Applied Computer Science, Kraków, Poland Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland National Center for Nuclear Research (NCBJ), Warsaw, Poland Horia Hulubei National Institute of Physics and Nuclear Engineering, Bucharest-Magurele, Romania Affiliated with an institute covered by a cooperation agreement with CERN DS4DS, La Salle, Universitat Ramon Llull, Barcelona, Spain ICCUB, Universitat de Barcelona, Barcelona, Spain Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain Instituto de Fisica Corpuscular, Centro Mixto Universidad de Valencia - CSIC, Valencia, Spain European Organization for Nuclear Research (CERN), Geneva, Switzerland Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland Physik-Institut, Universität Zürich, Zürich, Switzerland NSC Kharkiv Institute of Physics and Technology (NSC KIPT), Kharkiv, Ukraine Institute for Nuclear Research of the National Academy of Sciences (KINR), Kyiv, Ukraine University of Birmingham, Birmingham, United Kingdom H.H. Wills Physics Laboratory, University of Bristol, Bristol, United Kingdom Cavendish Laboratory, University of Cambridge, Cambridge, United Kingdom Department of Physics, University of Warwick, Coventry, United Kingdom STFC Rutherford Appleton Laboratory, Didcot, United Kingdom School of Physics and Astronomy, University of Edinburgh, Edinburgh, United Kingdom School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom Oliver Lodge Laboratory, University of Liverpool, Liverpool, United Kingdom Imperial College London, London, United Kingdom Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom Department of Physics, University of Oxford, Oxford, United Kingdom Massachusetts Institute of Technology, Cambridge, Massachusetts, USA University of Cincinnati, Cincinnati, Ohio, USA University of Maryland, College Park, Maryland, USA Los Alamos National Laboratory (LANL), Los Alamos, New Mexico, USA Syracuse University, Syracuse, New York, USA Pontifícia Universidade Católica do Rio de Janeiro (PUC-Rio), Rio de Janeiro, Brazil (associated with Universidade Federal do Rio de Janeiro (UFRJ), Rio de Janeiro, Brazil) School of Physics and Electronics, Hunan University, Changsha City, China (associated with Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China) Guangdong Provincial Key Laboratory of Nuclear Science, Guangdong-Hong Kong Joint Laboratory of Quantum Matter, Institute of Quantum Matter, South China Normal University, Guangzhou, China (associated with Center for High Energy Physics, Tsinghua University, Beijing, China) Lanzhou University, Lanzhou, China (associated with Institute Of High Energy Physics (IHEP), Beijing, China) School of Physics and Technology, Wuhan University, Wuhan, China (associated with Center for High Energy Physics, Tsinghua University, Beijing, China) Departamento de Fisica, Universidad Nacional de Colombia, Bogota, Colombia (associated with LPNHE, Sorbonne Université, Paris Diderot Sorbonne Paris Cité, CNRS/IN2P3, Paris, France) Universität Bonn - Helmholtz-Institut für Strahlen und Kernphysik, Bonn, Germany (associated with Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany) Eotvos Lorand University, Budapest, Hungary (associated with European Organization for Nuclear Research (CERN), Geneva, Switzerland) Van Swinderen Institute, University of Groningen, Groningen, Netherlands (associated with Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands) Universiteit Maastricht, Maastricht, Netherlands (associated with Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands) Tadeusz Kosciuszko Cracow University of Technology, Cracow, Poland (associated with Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland) Department of Physics and Astronomy, Uppsala University, Uppsala, Sweden (associated with School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom) University of Michigan, Ann Arbor, Michigan, USA (associated with Syracuse University, Syracuse, New York, USA) Departement de Physique Nucleaire (SPhN), Gif-Sur-Yvette, France
A T Grecu Horia Hulubei National Institute of Physics and Nuclear Engineering, Bucharest-Magurele, Romania
L M Greeven Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands
N A Grieser University of Cincinnati, Cincinnati, Ohio, USA
L Grillo School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom
S Gromov Affiliated with an institute covered by a cooperation agreement with CERN
C Gu Laboratoire Leprince-Ringuet, CNRS/IN2P3, Ecole Polytechnique, Institut Polytechnique de Paris, Palaiseau, France
M Guarise INFN Sezione di Ferrara, Ferrara, Italy
M Guittiere Université Paris-Saclay, CNRS/IN2P3, IJCLab, Orsay, France
V Guliaeva Affiliated with an institute covered by a cooperation agreement with CERN
P A Günther Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
A-K Guseinov Affiliated with an institute covered by a cooperation agreement with CERN
E Gushchin Affiliated with an institute covered by a cooperation agreement with CERN
Y Guz School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China Affiliated with an institute covered by a cooperation agreement with CERN European Organization for Nuclear Research (CERN), Geneva, Switzerland
T Gys European Organization for Nuclear Research (CERN), Geneva, Switzerland
T Hadavizadeh School of Physics and Astronomy, Monash University, Melbourne, Australia
C Hadjivasiliou University of Maryland, College Park, Maryland, USA
G Haefeli Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
C Haen European Organization for Nuclear Research (CERN), Geneva, Switzerland
J Haimberger European Organization for Nuclear Research (CERN), Geneva, Switzerland
M Hajheidari European Organization for Nuclear Research (CERN), Geneva, Switzerland
T Halewood-Leagas Oliver Lodge Laboratory, University of Liverpool, Liverpool, United Kingdom
M M Halvorsen European Organization for Nuclear Research (CERN), Geneva, Switzerland
P M Hamilton University of Maryland, College Park, Maryland, USA
J Hammerich Oliver Lodge Laboratory, University of Liverpool, Liverpool, United Kingdom
Q Han Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China
X Han Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
S Hansmann-Menzemer Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
L Hao University of Chinese Academy of Sciences, Beijing, China
N Harnew Department of Physics, University of Oxford, Oxford, United Kingdom
T Harrison Oliver Lodge Laboratory, University of Liverpool, Liverpool, United Kingdom
M Hartmann Université Paris-Saclay, CNRS/IN2P3, IJCLab, Orsay, France
C Hasse European Organization for Nuclear Research (CERN), Geneva, Switzerland
J He University of Chinese Academy of Sciences, Beijing, China
K Heijhoff Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands
F Hemmer European Organization for Nuclear Research (CERN), Geneva, Switzerland
C Henderson University of Cincinnati, Cincinnati, Ohio, USA
R D L Henderson School of Physics and Astronomy, Monash University, Melbourne, Australia Department of Physics, University of Warwick, Coventry, United Kingdom
A M Hennequin European Organization for Nuclear Research (CERN), Geneva, Switzerland
K Hennessy Oliver Lodge Laboratory, University of Liverpool, Liverpool, United Kingdom
L Henry Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
J Herd Imperial College London, London, United Kingdom
J Heuel I. Physikalisches Institut, RWTH Aachen University, Aachen, Germany
A Hicheur Universidade Federal do Rio de Janeiro (UFRJ), Rio de Janeiro, Brazil
D Hill Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
S E Hollitt Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
J Horswill Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
R Hou Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China
Y Hou Université Savoie Mont Blanc, CNRS, IN2P3-LAPP, Annecy, France
N Howarth Oliver Lodge Laboratory, University of Liverpool, Liverpool, United Kingdom
J Hu Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
J Hu Guangdong Provincial Key Laboratory of Nuclear Science, Guangdong-Hong Kong Joint Laboratory of Quantum Matter, Institute of Quantum Matter, South China Normal University, Guangzhou, China (associated with Center for High Energy Physics, Tsinghua University, Beijing, China)
W Hu School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China
X Hu Center for High Energy Physics, Tsinghua University, Beijing, China
W Huang University of Chinese Academy of Sciences, Beijing, China
W Hulsbergen Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands
R J Hunter Department of Physics, University of Warwick, Coventry, United Kingdom
M Hushchyn Affiliated with an institute covered by a cooperation agreement with CERN
D Hutchcroft Oliver Lodge Laboratory, University of Liverpool, Liverpool, United Kingdom
M Idzik AGH - University of Science and Technology, Faculty of Physics and Applied Computer Science, Kraków, Poland
D Ilin Affiliated with an institute covered by a cooperation agreement with CERN
P Ilten University of Cincinnati, Cincinnati, Ohio, USA
A Inglessi Affiliated with an institute covered by a cooperation agreement with CERN
A Iniukhin Affiliated with an institute covered by a cooperation agreement with CERN
A Ishteev Affiliated with an institute covered by a cooperation agreement with CERN
K Ivshin Affiliated with an institute covered by a cooperation agreement with CERN
R Jacobsson European Organization for Nuclear Research (CERN), Geneva, Switzerland
H Jage I. Physikalisches Institut, RWTH Aachen University, Aachen, Germany
S J Jaimes Elles Instituto de Fisica Corpuscular, Centro Mixto Universidad de Valencia - CSIC, Valencia, Spain Departamento de Fisica, Universidad Nacional de Colombia, Bogota, Colombia (associated with LPNHE, Sorbonne Université, Paris Diderot Sorbonne Paris Cité, CNRS/IN2P3, Paris, France)
S Jakobsen European Organization for Nuclear Research (CERN), Geneva, Switzerland
E Jans Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands
B K Jashal Instituto de Fisica Corpuscular, Centro Mixto Universidad de Valencia - CSIC, Valencia, Spain
A Jawahery University of Maryland, College Park, Maryland, USA
V Jevtic Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
E Jiang University of Maryland, College Park, Maryland, USA
X Jiang Institute Of High Energy Physics (IHEP), Beijing, China University of Chinese Academy of Sciences, Beijing, China
Y Jiang University of Chinese Academy of Sciences, Beijing, China
Y J Jiang School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China
M John Department of Physics, University of Oxford, Oxford, United Kingdom
D Johnson University of Birmingham, Birmingham, United Kingdom
C R Jones Cavendish Laboratory, University of Cambridge, Cambridge, United Kingdom
T P Jones Department of Physics, University of Warwick, Coventry, United Kingdom
S Joshi National Center for Nuclear Research (NCBJ), Warsaw, Poland
B Jost European Organization for Nuclear Research (CERN), Geneva, Switzerland
N Jurik European Organization for Nuclear Research (CERN), Geneva, Switzerland
I Juszczak Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland
D Kaminaris Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
S Kandybei NSC Kharkiv Institute of Physics and Technology (NSC KIPT), Kharkiv, Ukraine
Y Kang Center for High Energy Physics, Tsinghua University, Beijing, China
M Karacson European Organization for Nuclear Research (CERN), Geneva, Switzerland
D Karpenkov Affiliated with an institute covered by a cooperation agreement with CERN
M Karpov Affiliated with an institute covered by a cooperation agreement with CERN
A M Kauniskangas Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
J W Kautz University of Cincinnati, Cincinnati, Ohio, USA
F Keizer European Organization for Nuclear Research (CERN), Geneva, Switzerland
D M Keller Syracuse University, Syracuse, New York, USA
M Kenzie Cavendish Laboratory, University of Cambridge, Cambridge, United Kingdom
T Ketel Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands
B Khanji Syracuse University, Syracuse, New York, USA
A Kharisova Affiliated with an institute covered by a cooperation agreement with CERN
S Kholodenko INFN Sezione di Pisa, Pisa, Italy
G Khreich Université Paris-Saclay, CNRS/IN2P3, IJCLab, Orsay, France
T Kirn I. Physikalisches Institut, RWTH Aachen University, Aachen, Germany
V S Kirsebom Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
O Kitouni Massachusetts Institute of Technology, Cambridge, Massachusetts, USA
S Klaver Nikhef National Institute for Subatomic Physics and VU University Amsterdam, Amsterdam, Netherlands
N Kleijne INFN Sezione di Pisa, Pisa, Italy
K Klimaszewski National Center for Nuclear Research (NCBJ), Warsaw, Poland
M R Kmiec National Center for Nuclear Research (NCBJ), Warsaw, Poland
S Koliiev Institute for Nuclear Research of the National Academy of Sciences (KINR), Kyiv, Ukraine
L Kolk Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
A Konoplyannikov Affiliated with an institute covered by a cooperation agreement with CERN
P Kopciewicz AGH - University of Science and Technology, Faculty of Physics and Applied Computer Science, Kraków, Poland European Organization for Nuclear Research (CERN), Geneva, Switzerland
P Koppenburg Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands
M Korolev Affiliated with an institute covered by a cooperation agreement with CERN
I Kostiuk Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands
O Kot Institute for Nuclear Research of the National Academy of Sciences (KINR), Kyiv, Ukraine
S Kotriakhova School of Physics and Astronomy, Monash University, Melbourne, Australia Centro Brasileiro de Pesquisas Físicas (CBPF), Rio de Janeiro, Brazil Universidade Federal do Rio de Janeiro (UFRJ), Rio de Janeiro, Brazil Center for High Energy Physics, Tsinghua University, Beijing, China Institute Of High Energy Physics (IHEP), Beijing, China School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China University of Chinese Academy of Sciences, Beijing, China Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China Consejo Nacional de Rectores (CONARE), San Jose, Costa Rica Université Savoie Mont Blanc, CNRS, IN2P3-LAPP, Annecy, France Université Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France Aix Marseille Univ, CNRS/IN2P3, CPPM, Marseille, France Université Paris-Saclay, CNRS/IN2P3, IJCLab, Orsay, France Laboratoire Leprince-Ringuet, CNRS/IN2P3, Ecole Polytechnique, Institut Polytechnique de Paris, Palaiseau, France LPNHE, Sorbonne Université, Paris Diderot Sorbonne Paris Cité, CNRS/IN2P3, Paris, France I. Physikalisches Institut, RWTH Aachen University, Aachen, Germany Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany Max-Planck-Institut für Kernphysik (MPIK), Heidelberg, Germany Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany School of Physics, University College Dublin, Dublin, Ireland INFN Sezione di Bari, Bari, Italy INFN Sezione di Bologna, Bologna, Italy INFN Sezione di Ferrara, Ferrara, Italy INFN Sezione di Firenze, Firenze, Italy INFN Laboratori Nazionali di Frascati, Frascati, Italy INFN Sezione di Genova, Genova, Italy INFN Sezione di Milano, Milano, Italy INFN Sezione di Milano-Bicocca, Milano, Italy INFN Sezione di Cagliari, Monserrato, Italy Università degli Studi di Padova, Università e INFN, Padova, Padova, Italy INFN Sezione di Perugia, Perugia, Italy INFN Sezione di Pisa, Pisa, Italy INFN Sezione di Roma La Sapienza, Roma, Italy INFN Sezione di Roma Tor Vergata, Roma, Italy Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands Nikhef National Institute for Subatomic Physics and VU University Amsterdam, Amsterdam, Netherlands AGH - University of Science and Technology, Faculty of Physics and Applied Computer Science, Kraków, Poland Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland National Center for Nuclear Research (NCBJ), Warsaw, Poland Horia Hulubei National Institute of Physics and Nuclear Engineering, Bucharest-Magurele, Romania Affiliated with an institute covered by a cooperation agreement with CERN DS4DS, La Salle, Universitat Ramon Llull, Barcelona, Spain ICCUB, Universitat de Barcelona, Barcelona, Spain Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain Instituto de Fisica Corpuscular, Centro Mixto Universidad de Valencia - CSIC, Valencia, Spain European Organization for Nuclear Research (CERN), Geneva, Switzerland Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland Physik-Institut, Universität Zürich, Zürich, Switzerland NSC Kharkiv Institute of Physics and Technology (NSC KIPT), Kharkiv, Ukraine Institute for Nuclear Research of the National Academy of Sciences (KINR), Kyiv, Ukraine University of Birmingham, Birmingham, United Kingdom H.H. Wills Physics Laboratory, University of Bristol, Bristol, United Kingdom Cavendish Laboratory, University of Cambridge, Cambridge, United Kingdom Department of Physics, University of Warwick, Coventry, United Kingdom STFC Rutherford Appleton Laboratory, Didcot, United Kingdom School of Physics and Astronomy, University of Edinburgh, Edinburgh, United Kingdom School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom Oliver Lodge Laboratory, University of Liverpool, Liverpool, United Kingdom Imperial College London, London, United Kingdom Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom Department of Physics, University of Oxford, Oxford, United Kingdom Massachusetts Institute of Technology, Cambridge, Massachusetts, USA University of Cincinnati, Cincinnati, Ohio, USA University of Maryland, College Park, Maryland, USA Los Alamos National Laboratory (LANL), Los Alamos, New Mexico, USA Syracuse University, Syracuse, New York, USA Pontifícia Universidade Católica do Rio de Janeiro (PUC-Rio), Rio de Janeiro, Brazil (associated with Universidade Federal do Rio de Janeiro (UFRJ), Rio de Janeiro, Brazil) School of Physics and Electronics, Hunan University, Changsha City, China (associated with Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China) Guangdong Provincial Key Laboratory of Nuclear Science, Guangdong-Hong Kong Joint Laboratory of Quantum Matter, Institute of Quantum Matter, South China Normal University, Guangzhou, China (associated with Center for High Energy Physics, Tsinghua University, Beijing, China) Lanzhou University, Lanzhou, China (associated with Institute Of High Energy Physics (IHEP), Beijing, China) School of Physics and Technology, Wuhan University, Wuhan, China (associated with Center for High Energy Physics, Tsinghua University, Beijing, China) Departamento de Fisica, Universidad Nacional de Colombia, Bogota, Colombia (associated with LPNHE, Sorbonne Université, Paris Diderot Sorbonne Paris Cité, CNRS/IN2P3, Paris, France) Universität Bonn - Helmholtz-Institut für Strahlen und Kernphysik, Bonn, Germany (associated with Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany) Eotvos Lorand University, Budapest, Hungary (associated with European Organization for Nuclear Research (CERN), Geneva, Switzerland) Van Swinderen Institute, University of Groningen, Groningen, Netherlands (associated with Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands) Universiteit Maastricht, Maastricht, Netherlands (associated with Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands) Tadeusz Kosciuszko Cracow University of Technology, Cracow, Poland (associated with Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland) Department of Physics and Astronomy, Uppsala University, Uppsala, Sweden (associated with School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom) University of Michigan, Ann Arbor, Michigan, USA (associated with Syracuse University, Syracuse, New York, USA) Departement de Physique Nucleaire (SPhN), Gif-Sur-Yvette, France
A Kozachuk Affiliated with an institute covered by a cooperation agreement with CERN
P Kravchenko Affiliated with an institute covered by a cooperation agreement with CERN
L Kravchuk Affiliated with an institute covered by a cooperation agreement with CERN
M Kreps Department of Physics, University of Warwick, Coventry, United Kingdom
S Kretzschmar I. Physikalisches Institut, RWTH Aachen University, Aachen, Germany
P Krokovny Affiliated with an institute covered by a cooperation agreement with CERN
W Krupa Syracuse University, Syracuse, New York, USA
W Krzemien National Center for Nuclear Research (NCBJ), Warsaw, Poland
J Kubat Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
S Kubis Tadeusz Kosciuszko Cracow University of Technology, Cracow, Poland (associated with Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland)
W Kucewicz Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland
M Kucharczyk Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland
V Kudryavtsev Affiliated with an institute covered by a cooperation agreement with CERN
E Kulikova Affiliated with an institute covered by a cooperation agreement with CERN
A Kupsc Department of Physics and Astronomy, Uppsala University, Uppsala, Sweden (associated with School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom)
B K Kutsenko Aix Marseille Univ, CNRS/IN2P3, CPPM, Marseille, France
D Lacarrere European Organization for Nuclear Research (CERN), Geneva, Switzerland
A Lai INFN Sezione di Cagliari, Monserrato, Italy
A Lampis INFN Sezione di Cagliari, Monserrato, Italy
D Lancierini Physik-Institut, Universität Zürich, Zürich, Switzerland
C Landesa Gomez Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
J J Lane School of Physics and Astronomy, Monash University, Melbourne, Australia
R Lane H.H. Wills Physics Laboratory, University of Bristol, Bristol, United Kingdom
C Langenbruch Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
J Langer Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
O Lantwin Affiliated with an institute covered by a cooperation agreement with CERN
T Latham Department of Physics, University of Warwick, Coventry, United Kingdom
F Lazzari INFN Sezione di Pisa, Pisa, Italy
C Lazzeroni University of Birmingham, Birmingham, United Kingdom
R Le Gac Aix Marseille Univ, CNRS/IN2P3, CPPM, Marseille, France
S H Lee University of Michigan, Ann Arbor, Michigan, USA (associated with Syracuse University, Syracuse, New York, USA)
R Lefèvre Université Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France
A Leflat Affiliated with an institute covered by a cooperation agreement with CERN
S Legotin Affiliated with an institute covered by a cooperation agreement with CERN
M Lehuraux Department of Physics, University of Warwick, Coventry, United Kingdom
O Leroy Aix Marseille Univ, CNRS/IN2P3, CPPM, Marseille, France
T Lesiak Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland
B Leverington Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
A Li Center for High Energy Physics, Tsinghua University, Beijing, China
H Li Guangdong Provincial Key Laboratory of Nuclear Science, Guangdong-Hong Kong Joint Laboratory of Quantum Matter, Institute of Quantum Matter, South China Normal University, Guangzhou, China (associated with Center for High Energy Physics, Tsinghua University, Beijing, China)
K Li Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China
L Li Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
P Li European Organization for Nuclear Research (CERN), Geneva, Switzerland
P-R Li Lanzhou University, Lanzhou, China (associated with Institute Of High Energy Physics (IHEP), Beijing, China)
S Li Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China
T Li Institute Of High Energy Physics (IHEP), Beijing, China
T Li Guangdong Provincial Key Laboratory of Nuclear Science, Guangdong-Hong Kong Joint Laboratory of Quantum Matter, Institute of Quantum Matter, South China Normal University, Guangzhou, China (associated with Center for High Energy Physics, Tsinghua University, Beijing, China)
Y Li Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China
Y Li Institute Of High Energy Physics (IHEP), Beijing, China
Z Li Syracuse University, Syracuse, New York, USA
Z Lian Center for High Energy Physics, Tsinghua University, Beijing, China
X Liang Syracuse University, Syracuse, New York, USA
C Lin University of Chinese Academy of Sciences, Beijing, China
T Lin STFC Rutherford Appleton Laboratory, Didcot, United Kingdom
R Lindner European Organization for Nuclear Research (CERN), Geneva, Switzerland
V Lisovskyi Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
R Litvinov INFN Sezione di Cagliari, Monserrato, Italy
G Liu Guangdong Provincial Key Laboratory of Nuclear Science, Guangdong-Hong Kong Joint Laboratory of Quantum Matter, Institute of Quantum Matter, South China Normal University, Guangzhou, China (associated with Center for High Energy Physics, Tsinghua University, Beijing, China)
H Liu University of Chinese Academy of Sciences, Beijing, China
K Liu Lanzhou University, Lanzhou, China (associated with Institute Of High Energy Physics (IHEP), Beijing, China)
Q Liu University of Chinese Academy of Sciences, Beijing, China
S Liu Institute Of High Energy Physics (IHEP), Beijing, China University of Chinese Academy of Sciences, Beijing, China
Y Liu School of Physics and Astronomy, University of Edinburgh, Edinburgh, United Kingdom
Y Liu Lanzhou University, Lanzhou, China (associated with Institute Of High Energy Physics (IHEP), Beijing, China)
Y L Liu Imperial College London, London, United Kingdom
A Lobo Salvia ICCUB, Universitat de Barcelona, Barcelona, Spain
A Loi INFN Sezione di Cagliari, Monserrato, Italy
J Lomba Castro Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
T Long Cavendish Laboratory, University of Cambridge, Cambridge, United Kingdom
J H Lopes Universidade Federal do Rio de Janeiro (UFRJ), Rio de Janeiro, Brazil
A Lopez Huertas ICCUB, Universitat de Barcelona, Barcelona, Spain
S López Soliño Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
G H Lovell Cavendish Laboratory, University of Cambridge, Cambridge, United Kingdom
C Lucarelli INFN Sezione di Firenze, Firenze, Italy
D Lucchesi Università degli Studi di Padova, Università e INFN, Padova, Padova, Italy
S Luchuk Affiliated with an institute covered by a cooperation agreement with CERN
M Lucio Martinez Universiteit Maastricht, Maastricht, Netherlands (associated with Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands)
V Lukashenko Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands Institute for Nuclear Research of the National Academy of Sciences (KINR), Kyiv, Ukraine
Y Luo Center for High Energy Physics, Tsinghua University, Beijing, China
A Lupato Università degli Studi di Padova, Università e INFN, Padova, Padova, Italy
E Luppi INFN Sezione di Ferrara, Ferrara, Italy
K Lynch School of Physics, University College Dublin, Dublin, Ireland
X-R Lyu University of Chinese Academy of Sciences, Beijing, China
G M Ma Center for High Energy Physics, Tsinghua University, Beijing, China
R Ma University of Chinese Academy of Sciences, Beijing, China
S Maccolini Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
F Machefert Université Paris-Saclay, CNRS/IN2P3, IJCLab, Orsay, France
F Maciuc Horia Hulubei National Institute of Physics and Nuclear Engineering, Bucharest-Magurele, Romania
I Mackay Department of Physics, University of Oxford, Oxford, United Kingdom
L R Madhan Mohan Cavendish Laboratory, University of Cambridge, Cambridge, United Kingdom
M M Madurai University of Birmingham, Birmingham, United Kingdom
A Maevskiy Affiliated with an institute covered by a cooperation agreement with CERN
D Magdalinski Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands
D Maisuzenko Affiliated with an institute covered by a cooperation agreement with CERN
M W Majewski AGH - University of Science and Technology, Faculty of Physics and Applied Computer Science, Kraków, Poland
J J Malczewski Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland
S Malde Department of Physics, University of Oxford, Oxford, United Kingdom
B Malecki Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland European Organization for Nuclear Research (CERN), Geneva, Switzerland
L Malentacca European Organization for Nuclear Research (CERN), Geneva, Switzerland
A Malinin Affiliated with an institute covered by a cooperation agreement with CERN
T Maltsev Affiliated with an institute covered by a cooperation agreement with CERN
G Manca INFN Sezione di Cagliari, Monserrato, Italy
G Mancinelli Aix Marseille Univ, CNRS/IN2P3, CPPM, Marseille, France
C Mancuso Université Paris-Saclay, CNRS/IN2P3, IJCLab, Orsay, France INFN Sezione di Milano, Milano, Italy
R Manera Escalero ICCUB, Universitat de Barcelona, Barcelona, Spain
D Manuzzi INFN Sezione di Bologna, Bologna, Italy
D Marangotto INFN Sezione di Milano, Milano, Italy
J F Marchand Université Savoie Mont Blanc, CNRS, IN2P3-LAPP, Annecy, France
R Marchevski Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
U Marconi INFN Sezione di Bologna, Bologna, Italy
S Mariani European Organization for Nuclear Research (CERN), Geneva, Switzerland
C Marin Benito ICCUB, Universitat de Barcelona, Barcelona, Spain European Organization for Nuclear Research (CERN), Geneva, Switzerland
J Marks Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
A M Marshall H.H. Wills Physics Laboratory, University of Bristol, Bristol, United Kingdom
P J Marshall Oliver Lodge Laboratory, University of Liverpool, Liverpool, United Kingdom
G Martelli INFN Sezione di Perugia, Perugia, Italy
G Martellotti INFN Sezione di Roma La Sapienza, Roma, Italy
L Martinazzoli European Organization for Nuclear Research (CERN), Geneva, Switzerland
M Martinelli INFN Sezione di Milano-Bicocca, Milano, Italy
D Martinez Santos Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
F Martinez Vidal Instituto de Fisica Corpuscular, Centro Mixto Universidad de Valencia - CSIC, Valencia, Spain
A Massafferri Centro Brasileiro de Pesquisas Físicas (CBPF), Rio de Janeiro, Brazil
M Materok I. Physikalisches Institut, RWTH Aachen University, Aachen, Germany
R Matev European Organization for Nuclear Research (CERN), Geneva, Switzerland
A Mathad Physik-Institut, Universität Zürich, Zürich, Switzerland
V Matiunin Affiliated with an institute covered by a cooperation agreement with CERN
C Matteuzzi Syracuse University, Syracuse, New York, USA
K R Mattioli Laboratoire Leprince-Ringuet, CNRS/IN2P3, Ecole Polytechnique, Institut Polytechnique de Paris, Palaiseau, France
A Mauri Imperial College London, London, United Kingdom
E Maurice Laboratoire Leprince-Ringuet, CNRS/IN2P3, Ecole Polytechnique, Institut Polytechnique de Paris, Palaiseau, France
J Mauricio ICCUB, Universitat de Barcelona, Barcelona, Spain
P Mayencourt Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
M Mazurek European Organization for Nuclear Research (CERN), Geneva, Switzerland
M McCann Imperial College London, London, United Kingdom
L Mcconnell School of Physics, University College Dublin, Dublin, Ireland
T H McGrath Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
N T McHugh School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom
A McNab Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
R McNulty School of Physics, University College Dublin, Dublin, Ireland
B Meadows University of Cincinnati, Cincinnati, Ohio, USA
G Meier Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
D Melnychuk National Center for Nuclear Research (NCBJ), Warsaw, Poland
M Merk Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands Universiteit Maastricht, Maastricht, Netherlands (associated with Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands)
A Merli INFN Sezione di Milano, Milano, Italy
L Meyer Garcia Universidade Federal do Rio de Janeiro (UFRJ), Rio de Janeiro, Brazil
D Miao Institute Of High Energy Physics (IHEP), Beijing, China University of Chinese Academy of Sciences, Beijing, China
H Miao University of Chinese Academy of Sciences, Beijing, China
M Mikhasenko Universität Bonn - Helmholtz-Institut für Strahlen und Kernphysik, Bonn, Germany (associated with Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany)
D A Milanes Departamento de Fisica, Universidad Nacional de Colombia, Bogota, Colombia (associated with LPNHE, Sorbonne Université, Paris Diderot Sorbonne Paris Cité, CNRS/IN2P3, Paris, France)
A Minotti INFN Sezione di Milano-Bicocca, Milano, Italy
E Minucci Syracuse University, Syracuse, New York, USA
T Miralles Université Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France
S E Mitchell School of Physics and Astronomy, University of Edinburgh, Edinburgh, United Kingdom
B Mitreska Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
D S Mitzel Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
A Modak STFC Rutherford Appleton Laboratory, Didcot, United Kingdom
A Mödden Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
R A Mohammed Department of Physics, University of Oxford, Oxford, United Kingdom
R D Moise I. Physikalisches Institut, RWTH Aachen University, Aachen, Germany
S Mokhnenko Affiliated with an institute covered by a cooperation agreement with CERN
T Mombächer European Organization for Nuclear Research (CERN), Geneva, Switzerland
M Monk School of Physics and Astronomy, Monash University, Melbourne, Australia Department of Physics, University of Warwick, Coventry, United Kingdom
I A Monroy Departamento de Fisica, Universidad Nacional de Colombia, Bogota, Colombia (associated with LPNHE, Sorbonne Université, Paris Diderot Sorbonne Paris Cité, CNRS/IN2P3, Paris, France)
S Monteil Université Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France
A Morcillo Gomez Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
G Morello INFN Laboratori Nazionali di Frascati, Frascati, Italy
M J Morello INFN Sezione di Pisa, Pisa, Italy
M P Morgenthaler Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
J Moron AGH - University of Science and Technology, Faculty of Physics and Applied Computer Science, Kraków, Poland
A B Morris European Organization for Nuclear Research (CERN), Geneva, Switzerland
A G Morris Aix Marseille Univ, CNRS/IN2P3, CPPM, Marseille, France
R Mountain Syracuse University, Syracuse, New York, USA
H Mu Center for High Energy Physics, Tsinghua University, Beijing, China
Z M Mu School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China
E Muhammad Department of Physics, University of Warwick, Coventry, United Kingdom
F Muheim School of Physics and Astronomy, University of Edinburgh, Edinburgh, United Kingdom
M Mulder Van Swinderen Institute, University of Groningen, Groningen, Netherlands (associated with Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands)
K Müller Physik-Institut, Universität Zürich, Zürich, Switzerland
F Mũnoz-Rojas Consejo Nacional de Rectores (CONARE), San Jose, Costa Rica
R Murta Imperial College London, London, United Kingdom
P Naik Oliver Lodge Laboratory, University of Liverpool, Liverpool, United Kingdom
T Nakada Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
R Nandakumar STFC Rutherford Appleton Laboratory, Didcot, United Kingdom
T Nanut European Organization for Nuclear Research (CERN), Geneva, Switzerland
I Nasteva Universidade Federal do Rio de Janeiro (UFRJ), Rio de Janeiro, Brazil
M Needham School of Physics and Astronomy, University of Edinburgh, Edinburgh, United Kingdom
N Neri INFN Sezione di Milano, Milano, Italy
S Neubert Universität Bonn - Helmholtz-Institut für Strahlen und Kernphysik, Bonn, Germany (associated with Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany)
N Neufeld European Organization for Nuclear Research (CERN), Geneva, Switzerland
P Neustroev Affiliated with an institute covered by a cooperation agreement with CERN
R Newcombe Imperial College London, London, United Kingdom
J Nicolini Université Paris-Saclay, CNRS/IN2P3, IJCLab, Orsay, France Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
D Nicotra Universiteit Maastricht, Maastricht, Netherlands (associated with Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands)
E M Niel Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
N Nikitin Affiliated with an institute covered by a cooperation agreement with CERN
P Nogga Universität Bonn - Helmholtz-Institut für Strahlen und Kernphysik, Bonn, Germany (associated with Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany)
N S Nolte Massachusetts Institute of Technology, Cambridge, Massachusetts, USA
C Normand Université Savoie Mont Blanc, CNRS, IN2P3-LAPP, Annecy, France INFN Sezione di Cagliari, Monserrato, Italy
J Novoa Fernandez Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
G Nowak University of Cincinnati, Cincinnati, Ohio, USA
C Nunez University of Michigan, Ann Arbor, Michigan, USA (associated with Syracuse University, Syracuse, New York, USA)
H N Nur School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom
A Oblakowska-Mucha AGH - University of Science and Technology, Faculty of Physics and Applied Computer Science, Kraków, Poland
V Obraztsov Affiliated with an institute covered by a cooperation agreement with CERN
T Oeser I. Physikalisches Institut, RWTH Aachen University, Aachen, Germany
S Okamura INFN Sezione di Ferrara, Ferrara, Italy European Organization for Nuclear Research (CERN), Geneva, Switzerland
R Oldeman INFN Sezione di Cagliari, Monserrato, Italy
F Oliva School of Physics and Astronomy, University of Edinburgh, Edinburgh, United Kingdom
M Olocco Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
C J G Onderwater Universiteit Maastricht, Maastricht, Netherlands (associated with Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands)
R H O'Neil School of Physics and Astronomy, University of Edinburgh, Edinburgh, United Kingdom
J M Otalora Goicochea Universidade Federal do Rio de Janeiro (UFRJ), Rio de Janeiro, Brazil
T Ovsiannikova Affiliated with an institute covered by a cooperation agreement with CERN
P Owen Physik-Institut, Universität Zürich, Zürich, Switzerland
A Oyanguren Instituto de Fisica Corpuscular, Centro Mixto Universidad de Valencia - CSIC, Valencia, Spain
O Ozcelik School of Physics and Astronomy, University of Edinburgh, Edinburgh, United Kingdom
K O Padeken Universität Bonn - Helmholtz-Institut für Strahlen und Kernphysik, Bonn, Germany (associated with Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany)
B Pagare Department of Physics, University of Warwick, Coventry, United Kingdom
P R Pais Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
T Pajero Department of Physics, University of Oxford, Oxford, United Kingdom
A Palano INFN Sezione di Bari, Bari, Italy
M Palutan INFN Laboratori Nazionali di Frascati, Frascati, Italy
G Panshin Affiliated with an institute covered by a cooperation agreement with CERN
L Paolucci Department of Physics, University of Warwick, Coventry, United Kingdom
A Papanestis STFC Rutherford Appleton Laboratory, Didcot, United Kingdom
M Pappagallo INFN Sezione di Bari, Bari, Italy
L L Pappalardo INFN Sezione di Ferrara, Ferrara, Italy
C Pappenheimer University of Cincinnati, Cincinnati, Ohio, USA
C Parkes Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
B Passalacqua INFN Sezione di Ferrara, Ferrara, Italy
G Passaleva INFN Sezione di Firenze, Firenze, Italy
D Passaro INFN Sezione di Pisa, Pisa, Italy
A Pastore INFN Sezione di Bari, Bari, Italy
M Patel Imperial College London, London, United Kingdom
J Patoc Department of Physics, University of Oxford, Oxford, United Kingdom
C Patrignani INFN Sezione di Bologna, Bologna, Italy
C J Pawley Universiteit Maastricht, Maastricht, Netherlands (associated with Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands)
A Pellegrino Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands
M Pepe Altarelli INFN Laboratori Nazionali di Frascati, Frascati, Italy
S Perazzini INFN Sezione di Bologna, Bologna, Italy
D Pereima Affiliated with an institute covered by a cooperation agreement with CERN
A Pereiro Castro Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
P Perret Université Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France
A Perro European Organization for Nuclear Research (CERN), Geneva, Switzerland
K Petridis H.H. Wills Physics Laboratory, University of Bristol, Bristol, United Kingdom
A Petrolini INFN Sezione di Genova, Genova, Italy
S Petrucci School of Physics and Astronomy, University of Edinburgh, Edinburgh, United Kingdom
H Pham Syracuse University, Syracuse, New York, USA
L Pica INFN Sezione di Pisa, Pisa, Italy
M Piccini INFN Sezione di Perugia, Perugia, Italy
B Pietrzyk Université Savoie Mont Blanc, CNRS, IN2P3-LAPP, Annecy, France
G Pietrzyk Université Paris-Saclay, CNRS/IN2P3, IJCLab, Orsay, France
D Pinci INFN Sezione di Roma La Sapienza, Roma, Italy
F Pisani European Organization for Nuclear Research (CERN), Geneva, Switzerland
M Pizzichemi INFN Sezione di Milano-Bicocca, Milano, Italy
V Placinta Horia Hulubei National Institute of Physics and Nuclear Engineering, Bucharest-Magurele, Romania
M Plo Casasus Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
F Polci LPNHE, Sorbonne Université, Paris Diderot Sorbonne Paris Cité, CNRS/IN2P3, Paris, France European Organization for Nuclear Research (CERN), Geneva, Switzerland
M Poli Lener INFN Laboratori Nazionali di Frascati, Frascati, Italy
A Poluektov Aix Marseille Univ, CNRS/IN2P3, CPPM, Marseille, France
N Polukhina Affiliated with an institute covered by a cooperation agreement with CERN
I Polyakov European Organization for Nuclear Research (CERN), Geneva, Switzerland
E Polycarpo Universidade Federal do Rio de Janeiro (UFRJ), Rio de Janeiro, Brazil
S Ponce European Organization for Nuclear Research (CERN), Geneva, Switzerland
D Popov University of Chinese Academy of Sciences, Beijing, China
S Poslavskii Affiliated with an institute covered by a cooperation agreement with CERN
K Prasanth Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland
C Prouve Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
V Pugatch Institute for Nuclear Research of the National Academy of Sciences (KINR), Kyiv, Ukraine
V Puill Université Paris-Saclay, CNRS/IN2P3, IJCLab, Orsay, France
G Punzi INFN Sezione di Pisa, Pisa, Italy
H R Qi Center for High Energy Physics, Tsinghua University, Beijing, China
W Qian University of Chinese Academy of Sciences, Beijing, China
N Qin Center for High Energy Physics, Tsinghua University, Beijing, China
S Qu Center for High Energy Physics, Tsinghua University, Beijing, China
R Quagliani Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
R I Rabadan Trejo Department of Physics, University of Warwick, Coventry, United Kingdom
B Rachwal AGH - University of Science and Technology, Faculty of Physics and Applied Computer Science, Kraków, Poland
J H Rademacker H.H. Wills Physics Laboratory, University of Bristol, Bristol, United Kingdom
M Rama INFN Sezione di Pisa, Pisa, Italy
M Ramírez García University of Michigan, Ann Arbor, Michigan, USA (associated with Syracuse University, Syracuse, New York, USA)
M Ramos Pernas Department of Physics, University of Warwick, Coventry, United Kingdom
M S Rangel Universidade Federal do Rio de Janeiro (UFRJ), Rio de Janeiro, Brazil
F Ratnikov Affiliated with an institute covered by a cooperation agreement with CERN
G Raven Nikhef National Institute for Subatomic Physics and VU University Amsterdam, Amsterdam, Netherlands
M Rebollo De Miguel Instituto de Fisica Corpuscular, Centro Mixto Universidad de Valencia - CSIC, Valencia, Spain
F Redi European Organization for Nuclear Research (CERN), Geneva, Switzerland
J Reich H.H. Wills Physics Laboratory, University of Bristol, Bristol, United Kingdom
F Reiss Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
Z Ren University of Chinese Academy of Sciences, Beijing, China
P K Resmi Department of Physics, University of Oxford, Oxford, United Kingdom
R Ribatti INFN Sezione di Pisa, Pisa, Italy
G R Ricart Laboratoire Leprince-Ringuet, CNRS/IN2P3, Ecole Polytechnique, Institut Polytechnique de Paris, Palaiseau, France Departement de Physique Nucleaire (SPhN), Gif-Sur-Yvette, France
D Riccardi INFN Sezione di Pisa, Pisa, Italy
S Ricciardi STFC Rutherford Appleton Laboratory, Didcot, United Kingdom
K Richardson Massachusetts Institute of Technology, Cambridge, Massachusetts, USA
M Richardson-Slipper School of Physics and Astronomy, University of Edinburgh, Edinburgh, United Kingdom
K Rinnert Oliver Lodge Laboratory, University of Liverpool, Liverpool, United Kingdom
P Robbe Université Paris-Saclay, CNRS/IN2P3, IJCLab, Orsay, France
G Robertson School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom
E Rodrigues European Organization for Nuclear Research (CERN), Geneva, Switzerland Oliver Lodge Laboratory, University of Liverpool, Liverpool, United Kingdom
E Rodriguez Fernandez Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
J A Rodriguez Lopez Departamento de Fisica, Universidad Nacional de Colombia, Bogota, Colombia (associated with LPNHE, Sorbonne Université, Paris Diderot Sorbonne Paris Cité, CNRS/IN2P3, Paris, France)
E Rodriguez Rodriguez Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
A Rogovskiy STFC Rutherford Appleton Laboratory, Didcot, United Kingdom
D L Rolf European Organization for Nuclear Research (CERN), Geneva, Switzerland
A Rollings Department of Physics, University of Oxford, Oxford, United Kingdom
P Roloff European Organization for Nuclear Research (CERN), Geneva, Switzerland
V Romanovskiy Affiliated with an institute covered by a cooperation agreement with CERN
M Romero Lamas Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
A Romero Vidal Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
G Romolini INFN Sezione di Ferrara, Ferrara, Italy
F Ronchetti Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
M Rotondo INFN Laboratori Nazionali di Frascati, Frascati, Italy
S R Roy Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
M S Rudolph Syracuse University, Syracuse, New York, USA
T Ruf European Organization for Nuclear Research (CERN), Geneva, Switzerland
M Ruiz Diaz Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
R A Ruiz Fernandez Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
J Ruiz Vidal Department of Physics and Astronomy, Uppsala University, Uppsala, Sweden (associated with School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom)
A Ryzhikov Affiliated with an institute covered by a cooperation agreement with CERN
J Ryzka AGH - University of Science and Technology, Faculty of Physics and Applied Computer Science, Kraków, Poland
J J Saborido Silva Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
R Sadek Laboratoire Leprince-Ringuet, CNRS/IN2P3, Ecole Polytechnique, Institut Polytechnique de Paris, Palaiseau, France
N Sagidova Affiliated with an institute covered by a cooperation agreement with CERN
N Sahoo University of Birmingham, Birmingham, United Kingdom
B Saitta INFN Sezione di Cagliari, Monserrato, Italy
M Salomoni INFN Sezione di Milano-Bicocca, Milano, Italy
C Sanchez Gras Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands
I Sanderswood Instituto de Fisica Corpuscular, Centro Mixto Universidad de Valencia - CSIC, Valencia, Spain
R Santacesaria INFN Sezione di Roma La Sapienza, Roma, Italy
C Santamarina Rios Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
M Santimaria INFN Laboratori Nazionali di Frascati, Frascati, Italy
L Santoro Centro Brasileiro de Pesquisas Físicas (CBPF), Rio de Janeiro, Brazil
E Santovetti INFN Sezione di Roma Tor Vergata, Roma, Italy
A Saputi INFN Sezione di Ferrara, Ferrara, Italy European Organization for Nuclear Research (CERN), Geneva, Switzerland
D Saranin Affiliated with an institute covered by a cooperation agreement with CERN
G Sarpis School of Physics and Astronomy, University of Edinburgh, Edinburgh, United Kingdom
M Sarpis Universität Bonn - Helmholtz-Institut für Strahlen und Kernphysik, Bonn, Germany (associated with Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany)
A Sarti INFN Sezione di Roma La Sapienza, Roma, Italy
C Satriano INFN Sezione di Roma La Sapienza, Roma, Italy
A Satta INFN Sezione di Roma Tor Vergata, Roma, Italy
M Saur School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China
D Savrina Affiliated with an institute covered by a cooperation agreement with CERN
H Sazak Université Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France
L G Scantlebury Smead Department of Physics, University of Oxford, Oxford, United Kingdom
A Scarabotto LPNHE, Sorbonne Université, Paris Diderot Sorbonne Paris Cité, CNRS/IN2P3, Paris, France
S Schael I. Physikalisches Institut, RWTH Aachen University, Aachen, Germany
S Scherl Oliver Lodge Laboratory, University of Liverpool, Liverpool, United Kingdom
A M Schertz Eotvos Lorand University, Budapest, Hungary (associated with European Organization for Nuclear Research (CERN), Geneva, Switzerland)
M Schiller School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom
H Schindler European Organization for Nuclear Research (CERN), Geneva, Switzerland
M Schmelling Max-Planck-Institut für Kernphysik (MPIK), Heidelberg, Germany
B Schmidt European Organization for Nuclear Research (CERN), Geneva, Switzerland
S Schmitt I. Physikalisches Institut, RWTH Aachen University, Aachen, Germany
H Schmitz Universität Bonn - Helmholtz-Institut für Strahlen und Kernphysik, Bonn, Germany (associated with Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany)
O Schneider Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
A Schopper European Organization for Nuclear Research (CERN), Geneva, Switzerland
N Schulte Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
S Schulte Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
M H Schune Université Paris-Saclay, CNRS/IN2P3, IJCLab, Orsay, France
R Schwemmer European Organization for Nuclear Research (CERN), Geneva, Switzerland
G Schwering I. Physikalisches Institut, RWTH Aachen University, Aachen, Germany
B Sciascia INFN Laboratori Nazionali di Frascati, Frascati, Italy
A Sciuccati European Organization for Nuclear Research (CERN), Geneva, Switzerland
S Sellam Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
A Semennikov Affiliated with an institute covered by a cooperation agreement with CERN
M Senghi Soares Nikhef National Institute for Subatomic Physics and VU University Amsterdam, Amsterdam, Netherlands
A Sergi INFN Sezione di Genova, Genova, Italy
N Serra European Organization for Nuclear Research (CERN), Geneva, Switzerland Physik-Institut, Universität Zürich, Zürich, Switzerland
L Sestini Università degli Studi di Padova, Università e INFN, Padova, Padova, Italy
A Seuthe Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
Y Shang School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China
D M Shangase University of Michigan, Ann Arbor, Michigan, USA (associated with Syracuse University, Syracuse, New York, USA)
M Shapkin Affiliated with an institute covered by a cooperation agreement with CERN
I Shchemerov Affiliated with an institute covered by a cooperation agreement with CERN
L Shchutska Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
T Shears Oliver Lodge Laboratory, University of Liverpool, Liverpool, United Kingdom
L Shekhtman Affiliated with an institute covered by a cooperation agreement with CERN
Z Shen School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China
S Sheng Institute Of High Energy Physics (IHEP), Beijing, China University of Chinese Academy of Sciences, Beijing, China
V Shevchenko Affiliated with an institute covered by a cooperation agreement with CERN
B Shi University of Chinese Academy of Sciences, Beijing, China
E B Shields INFN Sezione di Milano-Bicocca, Milano, Italy
Y Shimizu Université Paris-Saclay, CNRS/IN2P3, IJCLab, Orsay, France
E Shmanin Affiliated with an institute covered by a cooperation agreement with CERN
R Shorkin Affiliated with an institute covered by a cooperation agreement with CERN
J D Shupperd Syracuse University, Syracuse, New York, USA
R Silva Coutinho Syracuse University, Syracuse, New York, USA
G Simi Università degli Studi di Padova, Università e INFN, Padova, Padova, Italy
S Simone INFN Sezione di Bari, Bari, Italy
N Skidmore Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
R Skuza Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
T Skwarnicki Syracuse University, Syracuse, New York, USA
M W Slater University of Birmingham, Birmingham, United Kingdom
J C Smallwood Department of Physics, University of Oxford, Oxford, United Kingdom
E Smith Massachusetts Institute of Technology, Cambridge, Massachusetts, USA
K Smith Los Alamos National Laboratory (LANL), Los Alamos, New Mexico, USA
M Smith Imperial College London, London, United Kingdom
A Snoch Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands
L Soares Lavra School of Physics and Astronomy, University of Edinburgh, Edinburgh, United Kingdom
M D Sokoloff University of Cincinnati, Cincinnati, Ohio, USA
F J P Soler School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom
A Solomin Affiliated with an institute covered by a cooperation agreement with CERN H.H. Wills Physics Laboratory, University of Bristol, Bristol, United Kingdom
A Solovev Affiliated with an institute covered by a cooperation agreement with CERN
I Solovyev Affiliated with an institute covered by a cooperation agreement with CERN
R Song School of Physics and Astronomy, Monash University, Melbourne, Australia
Y Song Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
Y Song Center for High Energy Physics, Tsinghua University, Beijing, China
Y S Song School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China
F L Souza De Almeida Syracuse University, Syracuse, New York, USA
B Souza De Paula Universidade Federal do Rio de Janeiro (UFRJ), Rio de Janeiro, Brazil
E Spadaro Norella INFN Sezione di Milano, Milano, Italy
E Spedicato INFN Sezione di Bologna, Bologna, Italy
J G Speer Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
E Spiridenkov Affiliated with an institute covered by a cooperation agreement with CERN
P Spradlin School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom
V Sriskaran European Organization for Nuclear Research (CERN), Geneva, Switzerland
F Stagni European Organization for Nuclear Research (CERN), Geneva, Switzerland
M Stahl European Organization for Nuclear Research (CERN), Geneva, Switzerland
S Stahl European Organization for Nuclear Research (CERN), Geneva, Switzerland
S Stanislaus Department of Physics, University of Oxford, Oxford, United Kingdom
E N Stein European Organization for Nuclear Research (CERN), Geneva, Switzerland
O Steinkamp Physik-Institut, Universität Zürich, Zürich, Switzerland
O Stenyakin Affiliated with an institute covered by a cooperation agreement with CERN
H Stevens Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
D Strekalina Affiliated with an institute covered by a cooperation agreement with CERN
Y Su University of Chinese Academy of Sciences, Beijing, China
F Suljik Department of Physics, University of Oxford, Oxford, United Kingdom
J Sun INFN Sezione di Cagliari, Monserrato, Italy
L Sun School of Physics and Technology, Wuhan University, Wuhan, China (associated with Center for High Energy Physics, Tsinghua University, Beijing, China)
Y Sun University of Maryland, College Park, Maryland, USA
P N Swallow University of Birmingham, Birmingham, United Kingdom
K Swientek AGH - University of Science and Technology, Faculty of Physics and Applied Computer Science, Kraków, Poland
F Swystun Department of Physics, University of Warwick, Coventry, United Kingdom
A Szabelski National Center for Nuclear Research (NCBJ), Warsaw, Poland
T Szumlak AGH - University of Science and Technology, Faculty of Physics and Applied Computer Science, Kraków, Poland
M Szymanski European Organization for Nuclear Research (CERN), Geneva, Switzerland
Y Tan Center for High Energy Physics, Tsinghua University, Beijing, China
S Taneja Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
M D Tat Department of Physics, University of Oxford, Oxford, United Kingdom
A Terentev Physik-Institut, Universität Zürich, Zürich, Switzerland
F Terzuoli INFN Sezione di Pisa, Pisa, Italy
F Teubert European Organization for Nuclear Research (CERN), Geneva, Switzerland
E Thomas European Organization for Nuclear Research (CERN), Geneva, Switzerland
D J D Thompson University of Birmingham, Birmingham, United Kingdom
H Tilquin Imperial College London, London, United Kingdom
V Tisserand Université Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France
S T'Jampens Université Savoie Mont Blanc, CNRS, IN2P3-LAPP, Annecy, France
M Tobin Institute Of High Energy Physics (IHEP), Beijing, China
L Tomassetti INFN Sezione di Ferrara, Ferrara, Italy
G Tonani INFN Sezione di Milano, Milano, Italy
X Tong School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China
D Torres Machado Centro Brasileiro de Pesquisas Físicas (CBPF), Rio de Janeiro, Brazil
L Toscano Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
D Y Tou Center for High Energy Physics, Tsinghua University, Beijing, China
C Trippl DS4DS, La Salle, Universitat Ramon Llull, Barcelona, Spain
G Tuci Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
N Tuning Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands
L H Uecker Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
A Ukleja AGH - University of Science and Technology, Faculty of Physics and Applied Computer Science, Kraków, Poland
D J Unverzagt Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
E Ursov Affiliated with an institute covered by a cooperation agreement with CERN
A Usachov Nikhef National Institute for Subatomic Physics and VU University Amsterdam, Amsterdam, Netherlands
A Ustyuzhanin Affiliated with an institute covered by a cooperation agreement with CERN
U Uwer Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
V Vagnoni INFN Sezione di Bologna, Bologna, Italy
A Valassi European Organization for Nuclear Research (CERN), Geneva, Switzerland
G Valenti INFN Sezione di Bologna, Bologna, Italy
N Valls Canudas DS4DS, La Salle, Universitat Ramon Llull, Barcelona, Spain
H Van Hecke Los Alamos National Laboratory (LANL), Los Alamos, New Mexico, USA
E van Herwijnen Imperial College London, London, United Kingdom
C B Van Hulse Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
R Van Laak Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
M van Veghel Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands
R Vazquez Gomez ICCUB, Universitat de Barcelona, Barcelona, Spain
P Vazquez Regueiro Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
C Vázquez Sierra Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
S Vecchi INFN Sezione di Ferrara, Ferrara, Italy
J J Velthuis H.H. Wills Physics Laboratory, University of Bristol, Bristol, United Kingdom
M Veltri INFN Sezione di Firenze, Firenze, Italy
A Venkateswaran Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
M Vesterinen Department of Physics, University of Warwick, Coventry, United Kingdom
D Vieira University of Cincinnati, Cincinnati, Ohio, USA
M Vieites Diaz European Organization for Nuclear Research (CERN), Geneva, Switzerland
X Vilasis-Cardona DS4DS, La Salle, Universitat Ramon Llull, Barcelona, Spain
E Vilella Figueras Oliver Lodge Laboratory, University of Liverpool, Liverpool, United Kingdom
A Villa INFN Sezione di Bologna, Bologna, Italy
P Vincent LPNHE, Sorbonne Université, Paris Diderot Sorbonne Paris Cité, CNRS/IN2P3, Paris, France
F C Volle Université Paris-Saclay, CNRS/IN2P3, IJCLab, Orsay, France
D Vom Bruch Aix Marseille Univ, CNRS/IN2P3, CPPM, Marseille, France
V Vorobyev Affiliated with an institute covered by a cooperation agreement with CERN
N Voropaev Affiliated with an institute covered by a cooperation agreement with CERN
K Vos Universiteit Maastricht, Maastricht, Netherlands (associated with Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands)
G Vouters Université Savoie Mont Blanc, CNRS, IN2P3-LAPP, Annecy, France
C Vrahas School of Physics and Astronomy, University of Edinburgh, Edinburgh, United Kingdom
J Walsh INFN Sezione di Pisa, Pisa, Italy
E J Walton School of Physics and Astronomy, Monash University, Melbourne, Australia
G Wan School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China
C Wang Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
G Wang Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China
J Wang School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China
J Wang Institute Of High Energy Physics (IHEP), Beijing, China
J Wang Center for High Energy Physics, Tsinghua University, Beijing, China
J Wang School of Physics and Technology, Wuhan University, Wuhan, China (associated with Center for High Energy Physics, Tsinghua University, Beijing, China)
M Wang INFN Sezione di Milano, Milano, Italy
N W Wang University of Chinese Academy of Sciences, Beijing, China
R Wang H.H. Wills Physics Laboratory, University of Bristol, Bristol, United Kingdom
X Wang Guangdong Provincial Key Laboratory of Nuclear Science, Guangdong-Hong Kong Joint Laboratory of Quantum Matter, Institute of Quantum Matter, South China Normal University, Guangzhou, China (associated with Center for High Energy Physics, Tsinghua University, Beijing, China)
X W Wang Imperial College London, London, United Kingdom
Y Wang Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China
Z Wang Université Paris-Saclay, CNRS/IN2P3, IJCLab, Orsay, France
Z Wang Center for High Energy Physics, Tsinghua University, Beijing, China
Z Wang University of Chinese Academy of Sciences, Beijing, China
J A Ward School of Physics and Astronomy, Monash University, Melbourne, Australia Department of Physics, University of Warwick, Coventry, United Kingdom
N K Watson University of Birmingham, Birmingham, United Kingdom
D Websdale Imperial College London, London, United Kingdom
Y Wei School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China
B D C Westhenry H.H. Wills Physics Laboratory, University of Bristol, Bristol, United Kingdom
D J White Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
M Whitehead School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom
A R Wiederhold Department of Physics, University of Warwick, Coventry, United Kingdom
D Wiedner Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
G Wilkinson Department of Physics, University of Oxford, Oxford, United Kingdom
M K Wilkinson University of Cincinnati, Cincinnati, Ohio, USA
M Williams Massachusetts Institute of Technology, Cambridge, Massachusetts, USA
M R J Williams School of Physics and Astronomy, University of Edinburgh, Edinburgh, United Kingdom
R Williams Cavendish Laboratory, University of Cambridge, Cambridge, United Kingdom
F F Wilson STFC Rutherford Appleton Laboratory, Didcot, United Kingdom
W Wislicki National Center for Nuclear Research (NCBJ), Warsaw, Poland
M Witek Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland
L Witola Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
C P Wong Los Alamos National Laboratory (LANL), Los Alamos, New Mexico, USA
G Wormser Université Paris-Saclay, CNRS/IN2P3, IJCLab, Orsay, France
S A Wotton Cavendish Laboratory, University of Cambridge, Cambridge, United Kingdom
H Wu Syracuse University, Syracuse, New York, USA
J Wu Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China
Y Wu School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China
K Wyllie European Organization for Nuclear Research (CERN), Geneva, Switzerland
S Xian Guangdong Provincial Key Laboratory of Nuclear Science, Guangdong-Hong Kong Joint Laboratory of Quantum Matter, Institute of Quantum Matter, South China Normal University, Guangzhou, China (associated with Center for High Energy Physics, Tsinghua University, Beijing, China)
Z Xiang Institute Of High Energy Physics (IHEP), Beijing, China
Y Xie Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China
A Xu INFN Sezione di Pisa, Pisa, Italy
J Xu University of Chinese Academy of Sciences, Beijing, China
L Xu Center for High Energy Physics, Tsinghua University, Beijing, China
L Xu Center for High Energy Physics, Tsinghua University, Beijing, China
M Xu Department of Physics, University of Warwick, Coventry, United Kingdom
Z Xu Université Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France
Z Xu University of Chinese Academy of Sciences, Beijing, China
Z Xu Institute Of High Energy Physics (IHEP), Beijing, China
D Yang Center for High Energy Physics, Tsinghua University, Beijing, China
S Yang University of Chinese Academy of Sciences, Beijing, China
X Yang School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China
Y Yang INFN Sezione di Genova, Genova, Italy
Z Yang School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China
Z Yang University of Maryland, College Park, Maryland, USA
V Yeroshenko Université Paris-Saclay, CNRS/IN2P3, IJCLab, Orsay, France
H Yeung Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
H Yin Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China
C Y Yu School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China
J Yu School of Physics and Electronics, Hunan University, Changsha City, China (associated with Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China)
X Yuan Institute Of High Energy Physics (IHEP), Beijing, China
E Zaffaroni Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
M Zavertyaev Max-Planck-Institut für Kernphysik (MPIK), Heidelberg, Germany
M Zdybal Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland
M Zeng Center for High Energy Physics, Tsinghua University, Beijing, China
C Zhang School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China
D Zhang Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China
J Zhang University of Chinese Academy of Sciences, Beijing, China
L Zhang Center for High Energy Physics, Tsinghua University, Beijing, China
S Zhang School of Physics and Electronics, Hunan University, Changsha City, China (associated with Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China)
S Zhang School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China
Y Zhang School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China
Y Zhang Department of Physics, University of Oxford, Oxford, United Kingdom
Y Z Zhang Center for High Energy Physics, Tsinghua University, Beijing, China
Y Zhao Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
A Zharkova Affiliated with an institute covered by a cooperation agreement with CERN
A Zhelezov Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
X Z Zheng Center for High Energy Physics, Tsinghua University, Beijing, China
Y Zheng University of Chinese Academy of Sciences, Beijing, China
T Zhou School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China
X Zhou Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China
Y Zhou University of Chinese Academy of Sciences, Beijing, China
V Zhovkovska Department of Physics, University of Warwick, Coventry, United Kingdom
L Z Zhu University of Chinese Academy of Sciences, Beijing, China
X Zhu Center for High Energy Physics, Tsinghua University, Beijing, China
X Zhu Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China
Z Zhu University of Chinese Academy of Sciences, Beijing, China
V Zhukov I. Physikalisches Institut, RWTH Aachen University, Aachen, Germany Affiliated with an institute covered by a cooperation agreement with CERN
J Zhuo Instituto de Fisica Corpuscular, Centro Mixto Universidad de Valencia - CSIC, Valencia, Spain
Q Zou Institute Of High Energy Physics (IHEP), Beijing, China University of Chinese Academy of Sciences, Beijing, China
D Zuliani Università degli Studi di Padova, Università e INFN, Padova, Padova, Italy
G Zunica Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom

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Prospects of targeting JAK/STAT signal transduction pathways for vasculitis

Vasculitis is the inflammation of blood vessels caused by autoimmunity and/or autoinflammation, and its etiology and pathogenesis remain largely unknown. The Janus kinase (JAK) and Signal transduction Transcription Activator (STAT) signal transduction pathways are a group of molecules involved in the major pathways by which many cytokines exert and integrate their functions, and their dysregulation has been implicated in the pathogenesis of a variety of autoimmune diseases. However, current data supporting the role of the JAK/STAT pathway in the development of vasculitis is limited. In terms of treatment, glucocorticoids and immunosuppressants have been the standard therapy. However, because of the huge burden of treatment side effects, people have long waited for new treatment options. JAK inhibitors reduce the production of multiple cytokines and inhibit inflammation by targeting the JAK/STAT pathway, and have the advantage of rapidly acting in oral formulations, reducing glucocorticoid dependence and associated adverse events, especially in refractory cases. Therefore, JAK inhibitors are expected to be a promising drug for the treatment of vasculitis.

Regulation of endogenous hormone and miRNA in leaves of alfalfa (Medicago sativa L.) seedlings under drought stress by endogenous nitric oxide

BACKGROUND

Alfalfa (Medicago sativa. L) is one of the best leguminous herbage in China and even in the world, with high nutritional and ecological value. However, one of the drawbacks of alfalfa is its sensitivity to dry conditions, which is a global agricultural problem. The objective of this study was to investigate the regulatory effects of endogenous nitric oxide (NO) on endogenous hormones and related miRNAs in alfalfa seedling leaves under drought stress. The effects of endogenous NO on endogenous hormones such as ABA, GA3, SA, and IAA in alfalfa leaves under drought stress were studied. In addition, high-throughput sequencing technology was used to identify drought-related miRNAs and endogenous NO-responsive miRNAs in alfalfa seedling leaves under drought stress.

RESULT

By measuring the contents of four endogenous hormones in alfalfa leaves, it was found that endogenous NO could regulate plant growth and stress resistance by inducing the metabolism levels of IAA, ABA, GA3, and SA in alfalfa, especially ABA and SA in alfalfa. In addition, small RNA sequencing technology and bioinformatics methods were used to analyze endogenous NO-responsive miRNAs under drought stress. It was found that most miRNAs were enriched in biological pathways and molecular functions related to hormones (ABA, ETH, and JA), phenylpropane metabolism, and plant stress tolerance.

CONCLUSION

In this study, the analysis of endogenous hormone signals and miRNAs in alfalfa leaves under PEG and PEG + cPTIO conditions provided an important basis for endogenous NO to improve the drought resistance of alfalfa at the physiological and molecular levels. It has important scientific value and practical significance for endogenous NO to improve plant drought resistance.

Ice-Templated Synthesis of Atomic Cluster Cocatalyst with Regulable Coordination Number for Enhanced Photocatalytic Hydrogen Evolution

Supported metal catalysts have been exploited in various applications. Among them, cocatalyst supported on photocatalyst is essential for activation of photocatalysis. However, cocatalyst decoration in a controllable fashion to promote intrinsic activity remains challenging. Herein, a versatile method is developed for cocatalyst synthesis using an ice-templating (ICT) strategy, resulting in size control from single-atom (SA), and atomic clusters (AC) to nanoparticles (NP). Importantly, the coordination numbers (CN) of decorated AC cocatalysts are highly controllable, and this ICT method applies to various metals and photocatalytic substrates. Taking narrow-band gap Ga-doped La5 Ti2 Cu0.9 Ag0.1 O7 S5 (LTCA) photocatalyst as an example, supported Ru AC/LTCA catalysts with regulable Ru CNs have been prepared, delivering significantly enhanced activities compared to Ru SA and Ru NPs supported on LTCA. Specifically, Ru(CN = 3.4) AC/LTCA with an average CN of Ru─Ru bond measured to be ≈3.4 exhibits excellent photocatalytic H2 evolution rate (578 µmol h-1 ) under visible light irradiation. Density functional theory calculation reveals that the modeled Ru(CN = 3) atomic cluster cocatalyst possesses favorable electronic properties and available active sites for the H2 evolution reaction.

Observation of Cabibbo-Suppressed Two-Body Hadronic Decays and Precision Mass Measurement of the Ω_{c}^{0} Baryon

The first observation of the singly Cabibbo-suppressed Ω_{c}^{0}→Ω^{-}K^{+} and Ω_{c}^{0}→Ξ^{-}π^{+} decays is reported, using proton-proton collision data at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 5.4  fb^{-1}, collected with the LHCb detector between 2016 and 2018. The branching fraction ratios are measured to be B(Ω_{c}^{0}→Ω^{-}K^{+})/B(Ω_{c}^{0}→Ω^{-}π^{+})=[6.08±0.51(stat)±0.40(syst)]%,B(Ω_{c}^{0}→Ξ^{-}π^{+})/B(Ω_{c}^{0}→Ω^{-}π^{+})=[15.81±0.87(stat)±0.44(syst)±0.16(ext)]%. In addition, using the Ω_{c}^{0}→Ω^{-}π^{+} decay channel, the Ω_{c}^{0} baryon mass is measured to be M(Ω_{c}^{0})=2695.28±0.07(stat)±0.27(syst)±0.30(ext)  MeV, improving the precision of the previous world average by a factor of 4.

Enhanced Production of Λ_{b}^{0} Baryons in High-Multiplicity pp Collisions at sqrt[s]=13 TeV

The production rate of Λ_{b}^{0} baryons relative to B^{0} mesons in pp collisions at a center-of-mass energy sqrt[s]=13  TeV is measured by the LHCb experiment. The ratio of Λ_{b}^{0} to B^{0} production cross sections shows a significant dependence on both the transverse momentum and the measured charged-particle multiplicity. At low multiplicity, the ratio measured at LHCb is consistent with the value measured in e^{+}e^{-} collisions, and increases by a factor of ∼2 with increasing multiplicity. At relatively low transverse momentum, the ratio of Λ_{b}^{0} to B^{0} cross sections is higher than what is measured in e^{+}e^{-} collisions, but converges with the e^{+}e^{-} ratio as the momentum increases. These results imply that the evolution of heavy b quarks into final-state hadrons is influenced by the density of the hadronic environment produced in the collision. Comparisons with several models and implications for the mechanisms enforcing quark confinement are discussed.

Highly sensitive detection of multiple antiviral drugs using graphitized hydroxylated multi-walled carbon nanotubes/ionic liquids-based electrochemical sensors

Global outbreaks and the spread of viral diseases in the recent years have led to a rapid increase in the usage of antiviral drugs (ATVs), the residues and metabolites of which are discharged into the natural environment, posing a serious threat to human health. There is an urgent need to develop sensitive and rapid detection tools for multiple ATVs. In this study, we developed a highly sensitive electrochemical sensor comprising a glassy carbon electrode (GCE) modified with graphitized hydroxylated multi-walled carbon nanotubes (G-MWCNT-OH) and 1-butyl-3-methylimidazolium hexafluorophosphate (BMIMPF6, IL) for the detection of six ATVs including famciclovir (FCV), remdesivir (REM), favipiravir (FAV), hydroxychloroquine sulfate (HCQ), cepharanthine (CEP) and molnupiravir (MOL). The morphology and structure of the G-MWCNT-OH/IL nanocomposites were characterized comprehensively, and the electroactive surface area and electron conductivity of G-MWCNT-OH/IL/GCE were determined using cyclic voltammetry and electrochemical impedance spectroscopy. The thermodynamic stability and non-covalent interactions between the G-MWCNT-OH and IL were evaluated through quantum chemical simulation calculations, and the mechanism of ATV detection using the G-MWCNT-OH/IL/GCE was thoroughly examined. The detection conditions were optimized to improve the sensitivity and stability of electrochemical sensors. Under the optimal experimental conditions, the G-MWCNT-OH/IL/GCE exhibited excellent electrocatalytic performance and detected the ATVs over a wide concentration range (0.01-120 μM). The limit of detections (LODs) were 42.3 nM, 55.4 nM, 21.9 nM, 15.6 nM, 10.6 nM, and 3.2 nM for FCV, REM, FAV, HCQ, CEP, and MOL, respectively. G-MWCNT-OH/IL/GCE was also highly stable and selective to the ATVs in the presence of multiple interfering analytes. This sensor exhibited great potential for enabling the quantitative detection of multiple ATVs in actual water environment.

Enfortumab vedotin and pembrolizumab as new first-line standard for metastatic urothelial cancer

Treatment options for patients with metastatic urothelial carcinoma ineligible for cisplatin-based chemotherapy have historically been limited. O'Donnell et al. recently reported the results of EV-103 Cohort K,1 leading to accelerated approval of enfortumab vedotin and pembrolizumab for cisplatin-ineligible patients and raising additional questions of how to best utilize this effective regimen.

The utility of behavioral biometrics in user authentication and demographic characteristic detection: a scoping review

BACKGROUND

Objective measures of screen time are necessary to better understand the complex relationship between screen time and health outcomes. However, current objective measures of screen time (e.g., passive sensing applications) are limited in identifying the user of the mobile device, a critical limitation in children's screen time research where devices are often shared across a family. Behavioral biometrics, a technology that uses embedded sensors on modern mobile devices to continuously authenticate users, could be used to address this limitation.

OBJECTIVE

The purpose of this scoping review was to summarize the current state of behavioral biometric authentication and synthesize these findings within the scope of applying behavioral biometric technology to screen time measurement.

METHODS

We systematically searched five databases (Web of Science Core Collection, Inspec in Engineering Village, Applied Science & Technology Source, IEEE Xplore, PubMed), with the last search in September of 2022. Eligible studies were on the authentication of the user or the detection of demographic characteristics (age, gender) using built-in sensors on mobile devices (e.g., smartphone, tablet). Studies were required to use the following methods for authentication: motion behavior, touch, keystroke dynamics, and/or behavior profiling. We extracted study characteristics (sample size, age, gender), data collection methods, data stream, model evaluation metrics, and performance of models, and additionally performed a study quality assessment. Summary characteristics were tabulated and compiled in Excel. We synthesized the extracted information using a narrative approach.

RESULTS

Of the 14,179 articles screened, 122 were included in this scoping review. Of the 122 included studies, the most highly used biometric methods were touch gestures (n = 76) and movement (n = 63), with 30 studies using keystroke dynamics and 6 studies using behavior profiling. Of the studies that reported age (47), most were performed exclusively in adult populations (n = 34). The overall study quality was low, with an average score of 5.5/14.

CONCLUSION

The field of behavioral biometrics is limited by the low overall quality of studies. Behavioral biometric technology has the potential to be used in a public health context to address the limitations of current measures of screen time; however, more rigorous research must be performed in child populations first.

SYSTEMATIC REVIEW REGISTRATION

The protocol has been pre-registered in the Open Science Framework database ( https://doi.org/10.17605/OSF.IO/92YCT ).

Improved Measurement of CP Violation Parameters in B_{s}^{0}→J/ψK^{+}K^{-} Decays in the Vicinity of the ϕ(1020) Resonance

The decay-time-dependent CP asymmetry in B_{s}^{0}→J/ψ(→μ^{+}μ^{-})K^{+}K^{-} decays is measured using proton-proton collision data, corresponding to an integrated luminosity of 6  fb^{-1}, collected with the LHCb detector at a center-of-mass energy of 13 TeV. Using a sample of approximately 349 000 B_{s}^{0} signal decays with an invariant K^{+}K^{-} mass in the vicinity of the ϕ(1020) resonance, the CP-violating phase ϕ_{s} is measured, along with the difference in decay widths of the light and heavy mass eigenstates of the B_{s}^{0}-B[over ¯]_{s}^{0} system, ΔΓ_{s}, and the difference of the average B_{s}^{0} and B^{0} meson decay widths, Γ_{s}-Γ_{d}. The values obtained are ϕ_{s}=-0.039±0.022±0.006  rad, ΔΓ_{s}=0.0845±0.0044±0.0024  ps^{-1}, and Γ_{s}-Γ_{d}=-0.0056_{-0.0015}^{+0.0013}±0.0014  ps^{-1}, where the first uncertainty is statistical and the second systematic. These are the most precise single measurements to date and are consistent with expectations based on the Standard Model and with the previous LHCb analyses of this decay. These results are combined with previous independent LHCb measurements. The phase ϕ_{s} is also measured independently for each polarization state of the K^{+}K^{-} system and shows no evidence for polarization dependence.

Efficacy of transcranial alternating current stimulation in treating chronic insomnia and the impact of age on its effectiveness: A multisite randomized, double-blind, parallel-group, placebo-controlled study

OBJECTIVE

Insomnia is a significant health issue associated with various systemic diseases. Transcranial alternating current stimulation (tACS) has been proposed as a potential intervention for insomnia. However, the efficacy and mechanisms of tACS in chronic insomnia remain unclear. Accordingly, this study aimed to investigate the efficacy of tACS in treating chronic insomnia in adults and assess the impact of age on its effectiveness using a large sample from two centers.

METHODS

A total of 120 participants with chronic insomnia underwent 20 daily sessions of tACS (duration: 40 min, frequency: 77.5 Hz, and intensity: 15 mA) or sham tACS targeting the forehead and both mastoid areas over 4 weeks. Assessments were conducted at baseline, post-treatment, and 4-week follow-up. Primary outcomes included sleep quality and efficiency, onset latency, total sleep time, and daily disturbances. Secondary outcomes included depression, anxiety, and clinical impression.

RESULTS

Compared with the control group, the tACS group demonstrated improved sleep quality and efficiency, increased total sleep time, and reduced daily disturbance (all ps < 0.01). Moreover, tACS had a significant effect on clinical impression (p < 0.001), but not depression and anxiety scores. Subgroup analyses revealed that older participants experienced significant benefits from tACS in sleep quality, efficiency, and overall insomnia reduction at post-treatment and follow-up (p < 0.001). Notably, improved insomnia correlated with attenuated depressive and anxiety symptoms.

CONCLUSIONS

These findings suggest that tACS may be an effective intervention for chronic insomnia within an eight-week timeframe, and age affects the response to tACS in terms of insomnia improvement.

The combination treatment of oncolytic adenovirus H101 with nivolumab for refractory advanced hepatocellular carcinoma: an open-label, single-arm, pilot study

BACKGROUND

H101, an innovative oncolytic adenovirus, has shown potential in modifying the tumor microenvironment from immunologically 'cold' to 'hot'. When combined with nivolumab, a programmed cell death protein 1 inhibitor, this synergy may offer substantial therapeutic benefits beyond the capabilities of each agent alone.

PATIENTS AND METHODS

In this pilot study, we assessed the efficacy and safety of combining H101 with nivolumab in advanced hepatocellular carcinoma (HCC) patients who failed prior systemic therapy. The participants received initial oncolytic virus (OV) pretreatment with intratumoral H101 injections (5.0 × 1011 vp/0.5 ml/vial, two vials per lesion) on days 1 and 3. Combination therapy started on day 8, with H101 administered every 2 or 4 weeks and nivolumab (240 mg) injections every 2 weeks. Treatment continued up to 12 months or until disease progression, intolerable toxicity, consent withdrawal, or study conclusion. The primary endpoint was the objective response rate (ORR).

RESULTS

Between March 2020 and March 2022, 18 of 21 screened patients were assessable, showing an ORR of 11.1% [two cases of partial response (PR) and five cases of stable disease], with extrahepatic injections often leading to favorable outcomes. The disease control rate stood at 38.9%, with a 6-month survival rate of 88.9%. Median progression-free survival was 2.69 months, and overall survival (OS) was 15.04 months. Common adverse events included low-grade fever (100%) and pain related to centesis (33.3%), and no grade 3/4 events were reported. Significantly, local H101 injection showed potential in reversing immune checkpoint inhibitor resistance, evidenced by over 2.5 years of extended OS in PR cases with low α-fetoprotein. Additionally, decreasing neutrophil-to-lymphocyte ratio during OV pretreatment may predict positive outcomes.

CONCLUSIONS

This study demonstrates the potential efficacy of combining H101 with nivolumab in treating refractory advanced HCC, with well-tolerated toxicities.

Intestinal Translocation of Live Porphyromonas gingivalis Drives Insulin Resistance

Periodontitis has been emphasized as a risk factor of insulin resistance-related systemic diseases. Accumulating evidence has suggested a possible "oral-gut axis" linking oral infection and extraoral diseases, but it remains unclear whether periodontal pathogens can survive the barriers of the digestive tract and how they play their pathogenic roles. The present study established a periodontitis mouse model through oral ligature plus Porphyromonas gingivalis inoculation and demonstrated that periodontitis aggravated diet-induced obesity and insulin resistance, while also causing P. gingivalis enrichment in the intestine. Metabolic labeling strategy validated that P. gingivalis could translocate to the gastrointestinal tract in a viable state. Oral administration of living P. gingivalis elicited insulin resistance, while administration of pasteurized P. gingivalis had no such effect. Combination analysis of metagenome sequencing and nontargeted metabolomics suggested that the tryptophan metabolism pathway, specifically indole and its derivatives, was involved in the pathogenesis of insulin resistance caused by oral administration of living P. gingivalis. Moreover, liquid chromatography-high-resolution mass spectrometry analysis confirmed that the aryl hydrocarbon receptor (AhR) ligands, mainly indole acetic acid, tryptamine, and indole-3-aldehyde, were reduced in diet-induced obese mice with periodontitis, leading to inactivation of AhR signaling. Supplementation with Ficz (6-formylindolo (3,2-b) carbazole), an AhR agonist, alleviated periodontitis-associated insulin resistance, in which the restoration of gut barrier function might play an important role. Collectively, these findings reveal that the oral-gut translocation of viable P. gingivalis works as a fuel linking periodontitis and insulin resistance, in which reduction of AhR ligands and inactivation of AhR signaling are involved. This study provides novel insight into the role of the oral-gut axis in the pathogenesis of periodontitis-associated comorbidities.

Measurement of CP Violation in B^{0}→ψ(→ℓ^{+}ℓ^{-})K_{S}^{0}(→π^{+}π^{-}) Decays

A measurement of time-dependent CP violation in the decays of B^{0} and B[over ¯]^{0} mesons to the final states J/ψ(→μ^{+}μ^{-})K_{S}^{0}, ψ(2S)(→μ^{+}μ^{-})K_{S}^{0} and J/ψ(→e^{+}e^{-})K_{S}^{0} with K_{S}^{0}→π^{+}π^{-} is presented. The data correspond to an integrated luminosity of 6  fb^{-1} collected at a center-of-mass energy of sqrt[s]=13  TeV with the LHCb detector. The CP-violation parameters are measured to be S_{ψK_{S}^{0}}=0.717±0.013(stat)±0.008(syst) and C_{ψK_{S}^{0}}=0.008±0.012(stat)±0.003(syst). This measurement of S_{ψK_{S}^{0}} represents the most precise single measurement of the CKM angle β to date and is more precise than the current world average. In addition, measurements of the CP-violation parameters of the individual channels are reported and a combination with the LHCb Run 1 measurements is performed.

Regional variations in retinopathy of prematurity incidence for preterm infants <32 weeks' gestation in China

OBJECTIVES

National-level data on the incidence of retinopathy of prematurity (ROP) in different regions of China is insufficient. This study aimed to compare ROP incidences and care practices in different regions of China and their relationship with regional gross domestic product (GDP) per capita.

STUDY DESIGN

Retrospective cohort study.

METHODS

All infants born at <32 weeks gestational age (GA) and admitted to 70 neonatal intensive care units (NICUs) from January 1, 2019, to December 31, 2020, were enrolled. Hospitals were categorised into three regional groups according to geographical locations and GDP per capita from high to low: Eastern, Central, and Western China. The incidence of death or ROP, and care practices were compared among the groups.

RESULTS

A total of 18,579 infants were enrolled. Median GA was 29.9 (interquartile range 28.4-31.0) weeks and birth weight was 1318.1 (317.2) g. The percentage of GA <28 weeks, complete administration of antenatal steroids, and weight gain velocity during NICU stay were highest in Eastern China and lowest in Western China (all P < 0.01). In Eastern, Central, and Western China, the rates of death or any stage of ROP were 33.3%, 38.5%, and 39.2%, respectively (P < 0.01).

CONCLUSIONS

There were considerable regional disparities in ROP incidence in preterm infants with GA <32 weeks in China. The incidence of death or ROP ranged from high to low in Western, Central, and Eastern China.

A remote sensing method for mapping alpine grasslines based on graph-cut

Climate change has induced substantial shifts in vegetation boundaries such as alpine treelines and shrublines, with widespread ecological and climatic influences. However, spatial and temporal changes in the upper elevational limit of alpine grasslands ("alpine grasslines") are still poorly understood due to lack of field observations and remote sensing estimates. In this study, taking the Tibetan Plateau as an example, we propose a novel method for automatically identifying alpine grasslines from multi-source remote sensing data and determining their positions at 30-m spatial resolution. We first identified 2895 mountains potentially having alpine grasslines. On each mountain, we identified a narrow area around the upper elevational limit of alpine grasslands where the alpine grassline was potentially located. Then, we used linear discriminant analysis to adaptively generate from Landsat reflectance features a synthetic feature that maximized the difference between vegetated and unvegetated pixels in each of these areas. After that, we designed a graph-cut algorithm to integrate the advantages of the Otsu and Canny approaches, which was used to determine the precise position of the alpine grassline from the synthetic feature image. Validation against alpine grasslines visually interpreted from a large number of high-spatial-resolution images showed a high level of accuracy (R2 , .99 and .98; mean absolute error, 22.6 and 36.2 m, vs. drone and PlanetScope images, respectively). Across the Tibetan Plateau, the alpine grassline elevation ranged from 4038 to 5380 m (5th-95th percentile), lower in the northeast and southeast and higher in the southwest. This study provides a method for remotely sensing alpine grasslines for the first-time at large scale and lays a foundation for investigating their responses to climate change.

Efficacy and Safety of Traditional Chinese Medicines as a Complementary Therapy Combined With Chemotherapy in the Treatment of Gastric Cancer: An Overview of Systematic Reviews and Meta-Analyses

BACKGROUND

In China, traditional Chinese medicines (TCMs), as a complementary therapy combined with chemotherapy, is widely used in the treatment of gastric cancer (GC). In order to systematically evaluate and synthesize existing evidence to provide a scientific basis for the efficacy and safety of this complementary therapy, we present an overview of systematic reviews (SRs) and meta-analyses (MAs) on the topic of TCMs as a complementary therapy in combination with chemotherapy for the treatment of GC.

METHODS

SRs/MAs on TCMs combined with chemotherapy for GC were comprehensively searched in 8 databases. Methodological quality, risk of bias, reporting quality, and quality of evidence were assessed using the Assessment of Multiple Systematic Reviews 2 (AMSTAR-2), the Risk of Bias in Systematic (ROBIS) scale, the Preferred Reporting Items for Systematic Reviews and Meta-Analyses 2020 (PRISMA 2020), as well as the Grading of Recommendations Assessment, Development, and Evaluation (GRADE) system.

RESULTS

Thirteen published SRs/MAs were included in our study. In terms of methodology, all SRs/MAs were considered to be of very low quality. Only 3 SRs/MAs has been assessed as low risk of bias. None of the SRs/MAs has been fully reported on the checklist. A total of 97 outcome indicators extracted from the included SRs/MAs were evaluated, and only 1 item was assessed as high quality.

CONCLUSIONS

TCMs may be an effective and safe complementary therapy in combination with chemotherapy for the treatment of GC. However, this conclusion must be treated with caution as the quality of the evidence provided by SRs/MAs is generally low.

A highly selective and sensitive electrochemical sensor for tetracycline resistant genes detection based on the non-covalent interaction of graphene oxide and nucleobase

Antibiotic resistance genes (ARGs) are causing worldwide environmental problems, however, the traditional analytical methods and test equipment for them are time-consuming and expensive. The electrochemical sensor using the non-covalent bond between graphene oxide (GO) and single-stranded tet (ss-tet) was established for specific tetracycline resistance genes (tet, composed of ss-tet and complementary ss-tet (ss-tet') in water) detection, which preparation time was only 35 min and far less than most reported sensors based on covalent bond. As the result of the detection for tet, the developed sensor not only had the low detection limit of 50.0 pM (8.1 × 102 copies·mL-1), the short detection time within 42 min, but also had satisfactory stability, excellent reproducibility, and highly selectivity (RSD < 4.43 %). Besides, it also had acceptable accuracy comparing to the real-time quantitative polymerase chain reaction (RT-qPCR) and PCR array in tet detection. Noticeably, it also had been successfully applied to tetA detection in different water samples. In brief, the prepared non-covalent bond sensor is simple, rapid, and suitable for highly selective and sensitive detection of the ARGs in actual water.

ASH2L, Core Subunit of H3K4 Methylation Complex, Regulates Amelogenesis

Histone methylation assumes a crucial role in the intricate process of enamel development. Our study has illuminated the substantial prevalence of H3K4me3 distribution, spanning from the cap stage to the late bell stage of dental germs. In order to delve into the role of H3K4me3 modification in amelogenesis and unravel the underlying mechanisms, we performed a conditional knockout of Ash2l, a core subunit essential for the establishment of H3K4me3 within the dental epithelium of mice. The absence of Ash2l resulted in reduced H3K4me3 modification, subsequently leading to abnormal morphology of dental germ at the late bell stage. Notably, knockout of Ash2l resulted in a loss of polarity in ameloblasts and odontoblasts. The proliferation and apoptosis of the inner enamel epithelium cells underwent dysregulation. Moreover, there was a notable reduction in the expression of matrix-related genes, Amelx and Dspp, accompanied with impaired enamel and dentin formation. Cut&Tag-seq (cleavage under targets and tagmentation sequencing) analysis substantiated a reduction of H3K4me3 modification on Shh, Trp63, Sp6, and others in the dental epithelium of Ash2l knockout mice. Validation through real-time polymerase chain reaction, immunohistochemistry, and immunofluorescence consistently affirmed the observed downregulation of Shh and Sp6 in the dental epithelium following Ash2l knockout. Intriguingly, the expression of Trp63 isomers, DNp63 and TAp63, was perturbed in Ash2l defect dental epithelium. Furthermore, the downstream target of TAp63, P21, exhibited aberrant expression within the cervical loop of mandibular first molars and incisors. Collectively, our findings suggest that ASH2L orchestrates the regulation of crucial amelogenesis-associated genes, such as Shh, Trp63, and others, by modulating H3K4me3 modification. Loss of ASH2L and H3K4me3 can lead to aberrant differentiation, proliferation, and apoptosis of the dental epithelium by affecting the expression of Shh, Trp63, and others genes, thereby contributing to the defects of amelogenesis.

In situ and General Multidentate Ligand Passivation Achieves Efficient and Ultra-Stable CsPbX3 Perovskite Quantum Dots for White Light-Emitting Diodes

Inorganic CsPbX3 perovskite quantum dots (PeQDs) show great potential in white light-emitting diodes (WLEDs) due to excellent optoelectronic properties, but their practical application is hampered by low photoluminescence quantum yield (PLQY) and especially poor stability. Herein,  we developed an in-situ and general multidentate ligand passivation strategy that allows for CsPbX3 PeQDs not only near-unit PLQY, but significantly improved stability against storage, heat, and polar solvent. The enhanced optical property arises from high effectiveness of the multidentate ligand, diethylenetriaminepentaacetic acid (DTPA) with five carboxyl groups, in passivating uncoordinated Pb2+ defects and suppressing nonradiative recombination. First-principles calculations reveal that the excellent stability is attributed to tridentate binding mode of DTPA that remarkably boosts the adsorption capacity to PeQD core. Finally, combining the green and red PeQDs with blue chip,  we demonstrated highly luminous WLEDs with distinctly enhanced operation stability, a wide color gamut of 121.3% of national television system committee, standard white light of (0.33,0.33) in CIE 1931, and tunable color temperatures from warm to cold white light readily by emitters' ratio. This study provides an operando yet general approach to achieve efficient and stable PeQDs for WLEDs and accelerates their progress to commercialization.

The Safety and Feasibility of Pulsed-Field Ablation in Atrioventricular Nodal Re-Entrant Tachycardia: First-in-Human Pilot Trial

BACKGROUND

The incidence of atrioventricular conduction system damage during the catheter ablation procedure has long been a safety concern in patients with atrioventricular nodal re-entrant tachycardia (AVNRT). Pulsed-field ablation (PFA) with high tissue selectivity is a promising technique to address this problem in patients with AVNRT.

OBJECTIVES

This study aimed to evaluate the safety and feasibility of PFA in patients with AVNRT.

METHODS

This was an investigator-initiated, single-center, single-arm, prospective study performed in West China Hospital, Sichuan University. Patients diagnosed with AVNRT by electrophysiological examination were included and treated using PFA. The primary outcome was the ability to achieve acute ablation success. The secondary outcomes were ablation success after 6 months and safety incidents reported.

RESULTS

A total of 30 patients with AVNRT with a mean age of 47.9 ± 13.9 years were included and underwent PFA. Acute ablation success was achieved in all patients. The skin-to-skin procedure time was 109.1 ± 32.1 minutes, and fluoroscopy time was 4.1 ± 0.9 minutes. A median of 8 (range: 6.5 to 11.0) PFA applications were delivered. The average distance of the closest ablation site to the His bundle was 6.5 ± 2.5 mm, with a minimum distance of 2.0 mm. All patients maintained sinus rhythm after 6 months. No adverse events occurred in any patient during the ablation or the 6-month follow-up.

CONCLUSIONS

PFA showed favorable feasibility and safety in patients with AVNRT in this pilot study. Further study with larger population and longer follow-up time is warranted to verify the results.

Genome-wide analysis of AP2/ERF gene and functional analysis of CqERF24 gene in drought stress in quinoa

Quinoa is a crop with high nutritional value and strong stress resistance. AP2/ERF transcription factors play a key role in plant growth and development. In this study, 148 AP2/ERF genes were identified in quinoa, which were divided into 5 subfamilies, including ERF, AP2, DREB, RAV and Soloist. The results showed that the number of introns ranged from 0 to 11, and the Motif 1-Motif 4 was highly conserved in most CqAP2/ERF proteins. The 148 CqAP2/ERF genes were distributed on 19 chromosomes. There were 93 pairs of duplicating genes in this family, and gene duplication played a critical role in the expansion of this family. Protein-protein interaction indicated that the proteins in CqAP2/ERF subfamily exhibited complex interactions, and GO enrichment analysis indicated that 148 CqAP2/ERF proteins were involved in transcription factor activity. In addition, CqAP2/ERF gene contains a large number of elements related to hormones in promoter region (IAA, GA, SA, ABA and MeJA) and stresses (salt, drought, low temperature and anaerobic induction). Transcriptome analysis under drought stress indicated that most of the CqAP2/ERF genes were responsive to drought stress, and subcellular localization indicated that CqERF24 was location in the nucleus, qRT-PCR results also showed that most of the genes such as CqERF15, CqERF24, CqDREB03, CqDREB14, CqDREB37 and CqDREB43 also responded to drought stress in roots and leaves. Overexpression of CqERF24 in Arabidopsis thaliana enhanced drought resistance by increasing antioxidant enzyme activity and activation-related stress genes, and the gene is sensitive to ABA, while silencing CqERF24 in quinoa decreased drought tolerance. In addition, overexpression of CqERF24 in quinoa calli enhanced resistance to mannitol. These results lay a solid foundation for further study on the role of AP2/ERF family genes in quinoa under drought stress.

Using CT imaging features to predict visceral pleural invasion of non-small-cell lung cancer

AIM

To examine the diagnostic performance of different models based on computed tomography (CT) imaging features in differentiating the invasiveness of non-small-cell lung cancer (NSCLC) with multiple pleural contact types.

MATERIALS AND METHODS

A total of 1,573 patients with NSCLC (tumour size ≤3 cm) were included retrospectively. The clinical and pathological data and preoperative imaging features of these patients were investigated and their relationships with visceral pleural invasion (VPI) were compared statistically. Multivariate logistic regression was used to eliminate confounding factors and establish different predictive models.

RESULTS

By univariate analysis and multivariable adjustment, surgical history, tumour marker (TM), number of pleural tags, length of solid contact and obstructive inflammation were identified as independent risk predictors of pleural invasiveness (p=0.014, 0.003, <0.001, <0.001, and 0.017, respectively). In the training group, comparison of the diagnostic efficacy between the combined model including these five independent predictors and the image feature model involving the latter three imaging predictors were as follows: sensitivity of 88.9% versus 77% and specificity of 73.5% versus 84.1%, with AUC of 0.868 (95% CI: 0.848-0.886) versus 0.862 (95% CI: 0.842-0.880; p=0.377). In the validation group, the sensitivity and specificity of these two models were as follow: the combined model, 93.5% and 74.3%, the imaging feature model, 77.4% and 81.3%, and their areas under the curve (AUCs) were both 0.884 (95% CI: 0.842-0.919). The best cut-off value of length of solid contact was 7.5 mm (sensitivity 68.9%, specificity 75.5%).

CONCLUSIONS

The image feature model showed great potential in predicting pleural invasiveness, and had comparable diagnostic efficacy compared with the combined model containing clinical data.

Sintilimab, bevacizumab biosimilar, and HAIC for unresectable hepatocellular carcinoma conversion therapy: a prospective, single-arm phase II trial

We assessed the efficacy and safety of sintilimab [an anti-programmed death (PD-1)] plus bevacizumab biosimilar (IBI305), and hepatic arterial infusion chemotherapy (HAIC) in patients with unresectable hepatocellular carcinoma (HCC). The patients received sintilimab (200 mg) plus IBI305 (7.5 mg/kg) and HAIC (FOLFOX for 23 h) and were treated every 3 weeks. The primary endpoint was the objective response rate (ORR) assessed by an independent review committee (IRC) per mRECIST v1.1. Twenty-nine patients were enrolled in our clinical trial (1 patient voluntarily withdrew due to adverse events after the initial treatment). Objective response was reached in 17/29 (58.6%) patients per mRECIST. A total of 19/29 (65.5%) patients became eligible for further treatment; 14 of them completed surgical resection; 1 (5.3%) achieved pathological complete response (pCR); and 5 (26.3%) reached major partial response (mPR). The 1-year OS rate was better in the PR or pCR+mPR+PR group than in the PD+SD group by either mRECIST or pathological assessment (p=0.039 and 0.006). The 1-year EFS rate was better in the PR group than in the PD+SD group by pathological assessment (p=0.007). The most common treatment-related adverse events (TEAEs) in 30 HCC patients included thrombocytopenia (40.0%), hypertension (23.3%), and leukopenia (23.3%). The grade 3-5 TEAEs that were observed were hypertension (10%), diarrhea (6.7%), asthenia (3.3%), and ascites (3.3%). Sintilimab plus IBI305 and HAIC showed promising efficacy and manageable safety in patients with unresectable HCC. It might represent a novel treatment option for these patients.

Hyperon Polarization along the Beam Direction Relative to the Second and Third Harmonic Event Planes in Isobar Collisions at sqrt[s_{NN}]=200 GeV

The polarization of Λ and Λ[over ¯] hyperons along the beam direction has been measured relative to the second and third harmonic event planes in isobar Ru+Ru and Zr+Zr collisions at sqrt[s_{NN}]=200  GeV. This is the first experimental evidence of the hyperon polarization by the triangular flow originating from the initial density fluctuations. The amplitudes of the sine modulation for the second and third harmonic results are comparable in magnitude, increase from central to peripheral collisions, and show a mild p_{T} dependence. The azimuthal angle dependence of the polarization follows the vorticity pattern expected due to elliptic and triangular anisotropic flow, and qualitatively disagrees with most hydrodynamic model calculations based on thermal vorticity and shear induced contributions. The model results based on one of existing implementations of the shear contribution lead to a correct azimuthal angle dependence, but predict centrality and p_{T} dependence that still disagree with experimental measurements. Thus, our results provide stringent constraints on the thermal vorticity and shear-induced contributions to hyperon polarization. Comparison to previous measurements at RHIC and the LHC for the second-order harmonic results shows little dependence on the collision system size and collision energy.

Promotion of Ca2+ Accumulation in Roots by Exogenous Brassinosteroids as a Key Mechanism for Their Enhancement of Plant Salt Tolerance: A Meta-Analysis and Systematic Review

Brassinosteroids (BRs), the sixth major phytohormone, can regulate plant salt tolerance. Many studies have been conducted to investigate the effects of BRs on plant salt tolerance, generating a large amount of research data. However, a meta-analysis on regulating plant salt tolerance by BRs has not been reported. Therefore, this study conducted a meta-analysis of 132 studies to elucidate the most critical physiological mechanisms by which BRs regulate salt tolerance in plants from a higher dimension and analyze the best ways to apply BRs. The results showed that exogenous BRs significantly increased germination, plant height, root length, and biomass (total dry weight was the largest) of plants under salt stress. There was no significant difference between seed soaking and foliar spraying. However, the medium method (germination stage) and stem application (seedling stage) may be more effective in improving plant salt tolerance. BRs only inhibit germination in Solanaceae. BRs (2 μM), seed soaking for 12 h, and simultaneous treatment with salt stress had the highest germination rate. At the seedling stage, the activity of Brassinolide (C28H48O6) was higher than that of Homobrassinolide (C29H50O6), and post-treatment, BRs (0.02 μM) was the best solution. BRs are unsuitable for use in the germination stage when Sodium chloride is below 100 mM, and the effect is also weakest in the seedling stage. Exogenous BRs promoted photosynthesis, and antioxidant enzyme activity increased the accumulation of osmoregulatory and antioxidant substances and reduced the content of harmful substances and Na+, thus reducing cell damage and improving plant salt tolerance. BRs induced the most soluble protein, chlorophyll a, stomatal conductance, net photosynthetic rate, Glutathione peroxidase, and root-Ca2+, with BRs causing Ca2+ signals in roots probably constituting the most important reason for improving salt tolerance. BRs first promoted the accumulation of Ca2+ in roots, which increased the content of the above vital substances and enzyme activities through the Ca2+ signaling pathway, improving plant salt tolerance.

Microfluidic-Assembled Covalent Organic Frameworks@Ti3 C2 Tx MXene Vertical Fibers for High-Performance Electrochemical Supercapacitors

The delicate design of innovative and sophisticated fibers with vertical porous skeleton and eminent electrochemical activity to generate directional ionic pathways and good faradic charge accessibility is pivotal but challenging for realizing high-performance fiber-shaped supercapacitors (FSCs). Here, hierarchically ordered hybrid fiber combined vertical-aligned and conductive Ti3 C2 Tx MXene (VA-Ti3 C2 Tx ) with interstratified electroactive covalent organic frameworks LZU1 (COF-LZU1) by one-step microfluidic synthesis is developed. Due to the incorporation of vertical channels, abundant redox active sites and large accessible surface area throughout the electrode, the VA-Ti3 C2 Tx @COF-LZU1 fibers express exceptional gravimetric capacitance of 787 F g-1 in a three-electrode system. Additionally, the solid-state asymmetric FSCs deliver a prominent energy density of 27 Wh kg-1 , capacitance of 398 F g-1 and cycling life of 20 000 cycles. The key to high energy storage ability originates from the decreased ions adsorption energy and ameliorative charge density distribution in vertically aligned and active hybrid fiber, accelerating ions transportation/accommodation and interfacial electrons transfer. Benefiting from excellent electrochemical performance, the FSCs offer sufficient energy supply to power watches, flags, and digital display tubes as well as be integrated with sensors to detect pulse signals, which opens a promising route for architecting advanced fiber toward the carbon neutrality market beyond energy-storage technology.

MRI features for prediction of the intravenous chemotherapy effect in patients with retinoblastoma

AIM

To investigate the value of orbital magnetic resonance imaging (MRI) features in predicting the efficacy of intravenous chemotherapy (IVC) for patients with retinoblastoma (RB).

MATERIALS AND METHODS

The pretreatment clinical and MRI data of 100 eyes from 80 RB patients who underwent IVC were collected retrospectively. There were 59 eyes in the effective group and 41 eyes in the ineffective group, and the baseline data of the two groups were compared statistically. Three radiologists reviewed and evaluated each lesion independently based on 25 MRI features. The predictive values of the MRI features for IVC efficacy were assessed by multi-factor logistic regression analysis, and their odds ratios (ORs) and 95% confidence intervals (95% CIs) were calculated. Receiver operating characteristic curves (ROCs) with the area under the curve (AUC) were used to determine the predictive abilities. A predictive model was constructed by integrating all independent predictors visualised by the nomogram.

RESULTS

There were no statistically significant differences in sex or age between the effective and ineffective groups. The results of multivariate regression analysis showed that laterality, margin, and anterior eye segment enhancement were identified as independent factors that could predict IVC efficacy. The predictive model combining these three features was constructed, and it had an AUC of 0.732 (95% CI: 0.633, 0.831, p<0.01), a sensitivity of 71.2%, and a specificity of 70.7%.

CONCLUSION

The data demonstrate that the orbital MRI features can be used to predict IVC efficiency before RB patients are treated.

Fabrication and 3D printing of Pickering emulsion gel based on Hypsizygus marmoreus by-products protein

Pickering emulsion gel (PEG) stabilized by the protein extracted from the by-product of Hypsizygus marmoreus, combining with xanthan gum (XG), was formulated as 3D printing ink. Hydrogen bonds are formed in XG/protein hybrid particles. Afterwards, PEG was developed. Results indicated that it has shear-thinning properties. The apparent viscosity, yield stress, Elastic modulus (G') and gel strength increased with the increased XG addition, while the size of emulsion decreased. XG incorporation improved the 3D printing performance with desired self-supporting capability and printing precision if its concentration reached 2.0% (w/v). This study provides ideas for the application of Hypsizygus marmoreus by-products protein in stabilizing PEG used for 3D printing, which has a potential to replace traditional hydrogenated cream for cake decoration.

Observation of New Baryons in the Ξ_{b}^{-}π^{+}π^{-} and Ξ_{b}^{0}π^{+}π^{-} Systems

The first observation and study of two new baryonic structures in the final state Ξ_{b}^{0}π^{+}π^{-} and the confirmation of the Ξ_{b}(6100)^{-} state in the Ξ_{b}^{-}π^{+}π^{-} decay mode are reported using proton-proton collision data collected by the LHCb experiment, corresponding to an integrated luminosity of 9  fb^{-1}. In addition, the properties of the known Ξ_{b}^{*0}, Ξ_{b}^{'-} and Ξ_{b}^{*-} resonances are measured with improved precision. The new decay mode of the Ξ_{b}^{0} baryon to the Ξ_{c}^{+} π^{-} π^{+} π^{-} final state is observed and exploited for the first time in these measurements.

Precision Measurement of CP Violation in the Penguin-Mediated Decay B_{s}^{0}→ϕϕ

A flavor-tagged time-dependent angular analysis of the decay B_{s}^{0}→ϕϕ is performed using pp collision data collected by the LHCb experiment at the center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 6  fb^{-1}. The CP-violating phase and direct CP-violation parameter are measured to be ϕ_{s}^{ss[over ¯]s}=-0.042±0.075±0.009  rad and |λ|=1.004±0.030±0.009, respectively, assuming the same values for all polarization states of the ϕϕ system. In these results, the first uncertainties are statistical and the second systematic. These parameters are also determined separately for each polarization state, showing no evidence for polarization dependence. The results are combined with previous LHCb measurements using pp collisions at center-of-mass energies of 7 and 8 TeV, yielding ϕ_{s}^{ss[over ¯]s}=-0.074±0.069  rad and |λ|=1.009±0.030. This is the most precise study of time-dependent CP violation in a penguin-dominated B meson decay. The results are consistent with CP symmetry and with the standard model predictions.

Non-targeted metabolomics analysis of metabolite changes in two quinoa genotypes under drought stress

BACKGROUND

Quinoa is an important economic crop, drought is one of the key factors affecting quinoa yield. Clarifying the adaptation strategy of quinoa to drought is conducive to cultivating drought-tolerant varieties. At present, the study of quinoa on drought stress-related metabolism and the identification of related metabolites are still unknown. As a direct feature of biochemical functions, metabolites can reveal the biochemical pathways involved in drought response.

RESULT

Here, we studied the physiological and metabolic responses of drought-tolerant genotype L1 and sensitive genotype HZ1. Under drought conditions, L1 had higher osmotic adjustment ability and stronger root activity than HZ1, and the relative water content of L1 was also higher than that of HZ1. In addition, the barrier-to- sea ratio of L1 is significantly higher than that of HZ1. Using untargeted metabolic analysis, a total of 523, 406, 301 and 272 differential metabolites were identified in L1 and HZ1 on day 3 and day 9 of drought stress. The key metabolites (amino acids, nucleotides, peptides, organic acids, lipids and carbohydrates) accumulated differently in quinoa leaves. and HZ1 had the most DEMs in Glycerophospholipid metabolism (ko00564) and ABC transporters (ko02010) pathways.

CONCLUSION

These results provide a reference for characterizing the response mechanism of quinoa to drought and improving the drought tolerance of quinoa.

Clinical characteristics of tuberculous meningitis in older patients compared with younger and middle-aged patients: a retrospective analysis

BACKGROUND

Few studies have analyzed the clinical characteristics and adverse factors affecting prognosis in older patients with tuberculous meningitis (TBM). This study aimed to compare the clinical characteristics of TBM in older patients with those in younger and middle-aged patients.

METHODS

This single-center retrospective study extracted data on the clinical features, cerebrospinal fluid changes, laboratory results, imaging features, and outcomes of patients with TBM from patient medical records and compared the findings in older patients (aged 60 years and older) with those of younger and middle-aged patients (aged 18-59 years).

RESULTS

The study included 197 patients with TBM, comprising 21 older patients aged 60-76 years at onset, and 176 younger and middle-aged patients aged 18-59 years at onset. Fever was common in both older (81%) and younger and middle-aged patients (79%). Compared with younger and middle-aged patients, older patients were more likely to have changes in awareness levels (67% vs. 40%), peripheral nerve dysfunction (57% vs. 29%), changes in cognitive function (48% vs. 20%), and focal seizures (33% vs. 6%), and less likely to have headache (71% vs. 93%), neck stiffness on meningeal stimulation (38% vs. 62%), and vomiting (47% vs. 68%). The Medical Research Council staging on admission of older patients was stage II (52%) and stage III (38%), whereas most younger and middle-aged patients had stage I (33%) and stage II (55%) disease. Neurological function evaluated on the 28th day of hospitalization was more likely to show poor prognosis in older patients than in younger and middle-aged patients (76% vs. 25%). Older patients had significantly higher red blood cell counts and blood glucose levels, and significantly lower serum albumin and sodium levels than those in younger and middle-aged patients. The cerebrospinal fluid protein levels, nucleated cell counts, glucose levels, and chloride levels did not differ significantly by age.

CONCLUSION

In patients with TBM, older patients have more severe clinical manifestations, a higher incidence of hydrocephalus and cerebral infarction, and longer hospital stays than younger and middle-aged patients. Older patients thus require special clinical attention.

Measurement of the Λ_{b}^{0}→Λ(1520)μ^{+}μ^{-} Differential Branching Fraction

The branching fraction of the rare decay Λ_{b}^{0}→Λ(1520)μ^{+}μ^{-} is measured for the first time, in the squared dimuon mass intervals q^{2}, excluding the J/ψ and ψ(2S) regions. The data sample analyzed was collected by the LHCb experiment at center-of-mass energies of 7, 8, and 13 TeV, corresponding to a total integrated luminosity of 9  fb^{-1}. The result in the highest q^{2} interval, q^{2}>15.0  GeV^{2}/c^{4}, where theoretical predictions have the smallest model dependence, agrees with the predictions.

Concurrent Chemoradiotherapy plus Programmed Death-1 (PD-1) Blockade for Locally Advanced Cervical Cancer: Preliminary Results of a Single-Arm, Open-Label, Phase II Trial

PURPOSE/OBJECTIVE(S)

This study aims to assess the anti-tumor activity and safety of concurrent chemoradiotherapy plus PD-1 blockade in patients with locally advanced cervical cancer.

MATERIALS/METHODS

This is a single-arm, open-label, prospective phase II study. The key inclusion criteria were treatment-naive patients aged 18-75 years with stage II A2-IVA (FIGO 2018) locally advanced cervical cancer. All patients were treated with concurrent chemoradiotherapy including 2 cycle cisplatin (75mg/m2, for three days, every 3 weeks[Q3W]), nedaplatin or carboplatin can be selected for patients who can't tolerate cisplatin. After CCRT, patients achieving complete response (CR), partial responses(PR), stable disease(SD) received adjuvant chemotherapy (docetaxel 75 mg/m2 day 1+ cisplatin DDP 25 mg/m2 day 1-3, Q3W) for 2 cycle. PD-1 blockade Sintilimab and Tislelizumab was administered intravenously at 200 mg every 3 weeks up to 1 year or until disease progression, unacceptable toxicity, or withdrawal of consent. The primary endpoint was objective response rate (ORR) assessed by investigators per Response Evaluation Criteria In Solid Tumours (RECIST) version 1.1. Secondary endpoints were the 12, 24-month overall survival (OS) rates, the 12, 24-month disease free survival (DFS) rates and safety.

RESULTS

From February 2020 to June 2022, a total of 15 patients was enrolled. Median age was 57 years (range, 36-74 years). Stage IIA1 was documented in 2 patients, stage IIA2 in two patients, stage IIIA in one patient, stage IIIC1 in eight patients, and stage IVA in two patients. And 66.7% (10/15) of patients had Metastatic lymph node. Four patients received adjuvant chemotherapy. The ORR was 100%, with 4 patients achieving CR and 11 PR. The 12 and 24-month OS rates are 93.3% and 84%, the 12 and 24-month DFS rates are 86% and 75.4%, respectively. Treatment-related adverse events (TRAEs) occurred in 86.7% (13/15) of patients. Grade 3 TRAEs are leukocyte (n = 1), thrombocytopenia (n = 1), hepatitis (n = 1), skin reaction (n = 1). No treatment-related deaths occurred. And IFN-γ was significantly elevated after radiotherapy (p = 0.0073).

CONCLUSION

Concurrent chemoradiotherapy plus PD-1 blockade showed promising antitumor activity and manageable toxicities in patients with locally advanced cervical cancer. Long-term outcomes are still pending to further evaluate their therapeutic effects. (ChiCTR2000032856).

Outcomes and Failure Patterns after Chemoradiotherapy for Locally Advanced Rectal Cancer with Positive Lateral Pelvic Lymph Nodes: A Propensity Score-Matched Analysis

PURPOSE/OBJECTIVE(S)

Locally advanced rectal cancer (LARC) combined with positive lateral pelvic lymph nodes (LPLN) tends to present worse prognosis. However, for those patients it remains unclear whether other combination high-risk factors affect the prognosis. This study aimed to use propensity score matching (PSM) to examine long-term outcomes and failure patterns in patients with positive vs. negative LPLN.

MATERIALS/METHODS

Patients with LARC were retrospectively divided into LPLN-positive and LPLN-negative groups. LPLN-positivity was defined as lymph node short diameter greater than or equal to 7 mm with specific morphological features. Clinical characteristics were compared between the groups using the chi-square test. PSM was applied to balance these differences. Progression-free survival (PFS) and overall survival (OS), and local-regional recurrence (LRR) and distant metastasis (DM) rates were compared between the groups using the Kaplan-Meier method and log-rank tests.

RESULTS

Prior to PSM, a total of 651 LARC patients were included. The LPLN-positive group had higher rates of lower location (53.1% vs. 43.0%, P = 0.025), mesorectal fascia (MRF)-positive (53.9% vs. 35.4%, P<0.001) and extramural venous invasion (EMVI)-positive (51.2% vs. 27.2%, P<0.001) disease than the LPLN-negative group. After PSM, there were 114 patients for each group along with the balanced clinical factors, and both groups had comparable surgery, pathologic complete response (pCR), and ypN stage rates. The median follow-up time was 45.9 months, 3-year OS (88.3% vs. 92.1%, P = 0.276) and LRR (5.7% vs. 2.8%, P = 0.172) rates were comparable between LPLN-positive and LPLN-negative groups. Meanwhile, despite no statistical difference, 3-year PFS (78.8% vs. 85.9%, P = 0.065) and DM (20.4% vs. 13.3%, P = 0.061) rates slightly differed between the groups. Among 10 patients with LRR, seven (70.0%) had lateral pelvic recurrence, among them, five patients were LPLN-positive, and four (80.0%) of these patients did not receive simultaneous integrated boost intensity-modulated radiotherapy (SIB- IMRT).45 patients were diagnosed with DM, 11 (40.7%) LPLN-positive and 3 (17.6%) LPLN-negative patients were diagnosed with oligometastases (P = 0.109).

CONCLUSION

Our study shows there is a tendency of worse PFS and DM in LPLN-positive than LPLN-negative patients, for LPLN-positive patients, oligometastases account for a large proportion of all distant metastases.

4D-MRI Guided Stereotactic Body Radiation Therapy for Unresectable Colorectal Liver Metastases

PURPOSE/OBJECTIVE(S)

This study evaluated the feasibilities and outcomes following four-dimensional magnetic resonance imaging (4D-MRI) guided stereotactic body radiation therapy (SBRT) for unresectable colorectal liver metastases (CRLM).

MATERIALS/METHODS

From March 2018 to January 2022, we identified 76 unresectable CRLM patients with 123 lesions who received 4D-MRI guided SBRT in our institution. 4D-MRI simulation with or without abdominal compression was conducted for all patients. The prescription dose was 50-65 Gy in 5-12 fractions. The image quality of computed tomography (CT) and MRI were compared using the Clarity Score. Clinical outcomes and toxicity profiles were evaluated.

RESULTS

The 4D-MRI significantly improved the image quality compared with CT images (mean Clarity Score: 1.67 vs 2.88, P < 0.001). The abdominal compression significantly reduced motions in cranial-caudal direction (P = 0.03) with 2 phase T2 weighted images assessing tumor motion. The median follow-up time was 12.5 months. For 98 lesions assessed for best response, the complete response, partial response and stable disease rate were 57.1 %, 30.6 % and 12.2 %, respectively. The local control (LC) rate at 2 year was 97.3%. 46.1% of patients experienced grade 1-2 toxicities and only 2.6% patients experienced grade 3 hematologic toxicities.

CONCLUSION

The 4D-MRI technique allowed precise target delineation and motion tracking in unresectable CRLM patients. High LC rate and mild toxicities were achieved. This study provided evidence for using 4D-MRI guided SBRT as an alternative treatment in unresectable CRLM.

30 Gy vs. 45 Gy Consolidative Thoracic Radiation (cTRT) for Extensive Stage Small Cell Lung Cancer (ES-SCLC): A Multicenter, Randomized, Phase 3 Trial

PURPOSE/OBJECTIVE(S)

Consolidative thoracic radiotherapy (cTRT) showed potential benefit to extensive stage small cell lung cancer (ES-SCLC). However, the optimum dose of cTRT is unknown. The purpose of this randomized trial was to compare the effect of 45 Gy in 15 fractions with 30 Gy in 10 fractions cTRT in ES-SCLC.

MATERIALS/METHODS

This phase III, randomized trial was conducted in 12 public hospitals in China. Eligible patients with pathologically confirmed ES-SCLC who responded to 4-6 cycles of etoposide plus cisplatin (EP) or carboplatin (EC) chemotherapy were randomized 1:1 to receive either 30 Gy in 10 fractions or 45 Gy in 15 fractions cTRT. The primary outcome was 2-year overall survival (OS). Secondary outcomes included 2-year progression-free survival (PFS), 2-year local control (LC) and radiation treatment related toxicity. The primary objective was to detect an OS improvement in 45 Gy cTRT group at 2 years from 13% to 26% assuming a two-sided a = 0.05 and power of 85%, with a planned sample size of 186 patients. This trial was registered with Clinical Trials.gov, number NCT02675088.

RESULTS

Between January 15, 2016, and September 20, 2022, 90 patients were randomly assigned either 30 Gy in 10 fractions (n = 50) or 45 Gy in 15 fractions (n = 40) cTRT group. Recruitment to the trial closed early due to slow accrual since first-line chemoimmunotherapy has become the new standard of care for ES-SCLC. The median age of patients was 58 years, 87.8% were male, 76.7% had a smoking history, 95.6% received IMRT, and 58.9% received prophylactic cranial irradiation. At a median follow-up of 39.9 months (IQR 27.2-59.2), there was no significant difference in the 2-year OS between the 45 Gy group and the 30 Gy group, at 43.4% (95% CI 29.3%-64.3%) and 40.0% (95% CI 27.9%-59.1%), respectively (log-rank p = 0.62; HR 1.13 [95% CI 0.69-1.84]). The 2-year PFS was 12.1% (95% CI 4.3%-33.8%) in the 45 Gy group and 9.0% (95% CI 3.2%-25.2%) in the 30 Gy group (log-rank p = 0.25, HR 0.76(95% CI [0.478-1.22]). There were also no significant differences in locoregional recurrence free survival (log-rank p = 0.75; HR 0.888 [95% CI 0.423-1.863]) and distant metastasis free survival (log-rank p = 0.95; HR 1.015 [95% CI 0.624-1.651]) between two groups. No grade 5 toxicity was observed in both groups. Patients treated with higher cTRT dose presented with increased incidence of grade 3+ radiation pneumonitis (10% vs 2%) and hematological toxicity (20% vs 12.5%).

CONCLUSION

This randomized trial did not find a higher probability of survival improvement in patients with ES-SCLC receiving cTRT of 45 Gy in 15 fractions compared with 30 Gy in 10 fractions. In contrast, there was an increase in toxicity, especially radiation pneumonitis. Additional randomized studies investigating the role of cTRT in ES-SCLC after a response to chemoimmunotherapy are warranted.