Identification of individual goat animals by means of near infrared spectroscopy and chemometrics analysis of commercial meat cuts

Although the identification of animal species and muscles have been reported previously, no studies have been found on the use of NIR spectroscopy to identify individual animals from the analysis of commercial meat cuts. The aim of this study was to evaluate the use of a portable near infrared (NIR) instrument combined with classical chemometrics methods [principal component analysis (PCA) and partial least squares discriminant analysis PLS-DA)] to identify the origin of individual goat animals using the spectral signature of their commercial cut. Samples were collected from several carcasses (6 commercial cuts x 24 animals) sourced from a commercial abattoir in Queensland (Australia). The NIR spectra of the samples were collected using a portable NIR instrument in the wavelength range between 950 and 1600 nm. Overall, the PLS-DA models correctly classify 82% and 79% of the individual goat samples using either the goat rack or loin cut samples, respectively. The study demonstrated that NIR spectroscopy was able to identify individual goat animals based on the spectra properties of some of the commercial cut samples analysed (e.g. loin and rack). These results showed the potential of this technique to identify individual animals as an alternative to other laboratory methods and techniques commonly used in meat traceability.

Investigating autophagy and intricate cellular mechanisms in hepatocellular carcinoma: Emphasis on cell death mechanism crosstalk

Hepatocellular carcinoma (HCC) stands as a formidable global health challenge due to its prevalence, marked by high mortality and morbidity rates. This cancer type exhibits a multifaceted etiology, prominently linked to viral infections, non-alcoholic fatty liver disease, and genomic mutations. The inherent heterogeneity of HCC, coupled with its proclivity for developing drug resistance, presents formidable obstacles to effective therapeutic interventions. Autophagy, a fundamental catabolic process, plays a pivotal role in maintaining cellular homeostasis, responding to stressors such as nutrient deprivation. In the context of HCC, tumor cells exploit autophagy, either augmenting or impeding its activity, thereby influencing tumorigenesis. This comprehensive review underscores the dualistic role of autophagy in HCC, acting as both a pro-survival and pro-death mechanism, impacting the trajectory of tumorigenesis. The anti-carcinogenic potential of autophagy is evident in its ability to enhance apoptosis and ferroptosis in HCC cells. Pertinently, dysregulated autophagy fosters drug resistance in the carcinogenic context. Both genomic and epigenetic factors can regulate autophagy in HCC progression. Recognizing the paramount importance of autophagy in HCC progression, this review introduces pharmacological compounds capable of modulating autophagy-either inducing or inhibiting it, as promising avenues in HCC therapy.

Human-multimodal deep learning collaboration in 'precise' diagnosis of lupus erythematosus subtypes and similar skin diseases

BACKGROUND

Lupus erythematosus (LE) is a spectrum of autoimmune diseases. Due to the complexity of cutaneous LE (CLE), clinical skin image-based artificial intelligence is still experiencing difficulties in distinguishing subtypes of LE.

OBJECTIVES

We aim to develop a multimodal deep learning system (MMDLS) for human-AI collaboration in diagnosis of LE subtypes.

METHODS

This is a multi-centre study based on 25 institutions across China to assist in diagnosis of LE subtypes, other eight similar skin diseases and healthy subjects. In total, 446 cases with 800 clinical skin images, 3786 multicolor-immunohistochemistry (multi-IHC) images and clinical data were collected, and EfficientNet-B3 and ResNet-18 were utilized in this study.

RESULTS

In the multi-classification task, the overall performance of MMDLS on 13 skin conditions is much higher than single or dual modals (Sen = 0.8288, Spe = 0.9852, Pre = 0.8518, AUC = 0.9844). Further, the MMDLS-based diagnostic-support help improves the accuracy of dermatologists from 66.88% ± 6.94% to 81.25% ± 4.23% (p = 0.0004).

CONCLUSIONS

These results highlight the benefit of human-MMDLS collaborated framework in telemedicine by assisting dermatologists and rheumatologists in the differential diagnosis of LE subtypes and similar skin diseases.

68Ga-NC-BCH Whole-Body PET Imaging Rapidly Targets Claudin18.2 in Lesions in Gastrointestinal Cancer Patients

68Ga-labeled nanobody (68Ga-NC-BCH) is a single-domain antibody-based PET imaging agent. We conducted a first-in-humans study of 68Ga-NC-BCH for PET to determine its in vivo biodistribution, metabolism, radiation dosimetry, safety, and potential for quantifying claudin-18 isoform 2 (CLDN18.2) expression in gastrointestinal cancer patients. Methods: Initially, we synthesized the probe 68Ga-NC-BCH and performed preclinical evaluations on human gastric adenocarcinoma cell lines and xenograft mouse models. Next, we performed a translational study with a pilot cohort of patients with advanced gastrointestinal cancer on a total-body PET/CT scanner. Radiopharmaceutical biodistribution, radiation dosimetry, and the relationship between tumor uptake and CLDN18.2 expression were evaluated. Results: 68Ga-NC-BCH was stably prepared and demonstrated good radiochemical properties. According to preclinical evaluation,68Ga-NC-BCH exhibited rapid blood clearance, high affinity for CLDN18.2, and high specific uptake in CLDN18.2-positive cells and xenograft mouse models. 68Ga-NC-BCH displayed high uptake in the stomach and kidney and slight uptake in the pancreas. Compared with 18F-FDG, 68Ga-NC-BCH showed significant differences in uptake in lesions with different levels of CLDN18.2 expression. Conclusion: A clear correlation was detected between PET SUV and CLDN18.2 expression, suggesting that 68Ga-NC-BCH PET could be used as a companion diagnostic tool for optimizing treatments that target CLDN18.2 in tumors.

A hybrid particle swarm optimization algorithm for solving engineering problem

To overcome the disadvantages of premature convergence and easy trapping into local optimum solutions, this paper proposes an improved particle swarm optimization algorithm (named NDWPSO algorithm) based on multiple hybrid strategies. Firstly, the elite opposition-based learning method is utilized to initialize the particle position matrix. Secondly, the dynamic inertial weight parameters are given to improve the global search speed in the early iterative phase. Thirdly, a new local optimal jump-out strategy is proposed to overcome the "premature" problem. Finally, the algorithm applies the spiral shrinkage search strategy from the whale optimization algorithm (WOA) and the Differential Evolution (DE) mutation strategy in the later iteration to accelerate the convergence speed. The NDWPSO is further compared with other 8 well-known nature-inspired algorithms (3 PSO variants and 5 other intelligent algorithms) on 23 benchmark test functions and three practical engineering problems. Simulation results prove that the NDWPSO algorithm obtains better results for all 49 sets of data than the other 3 PSO variants. Compared with 5 other intelligent algorithms, the NDWPSO obtains 69.2%, 84.6%, and 84.6% of the best results for the benchmark function (f 1 - f 13 ) with 3 kinds of dimensional spaces (Dim = 30,50,100) and 80% of the best optimal solutions for 10 fixed-multimodal benchmark functions. Also, the best design solutions are obtained by NDWPSO for all 3 classical practical engineering problems.

[Interaction between implants and natural teeth in patients with severe periodontitis:a retrospective study]

Objective: To evaluate the clinical outcomes after implant restoration in the posterior region of severe periodontitis patients and to investigate the factors of natural tooth affecting the implant from the perspective of improving natural periodontal health, which may provide a reference for clinical practice. Methods: Fifty-three patients with severe periodontitis who visited the Department of Periodontology at the Affiliated Stomatological Hospital of China Medical University from June 2014 to June 2023 and completed posterior implant treatment with single crown were included, among which were 16 males and 37 females, aged (52.2±8.0) years old, with a total of 136 implants, 135 adjacent natural teeth in the edentulous area. We retrospectively compared the changes of probing depth (PD), bleeding on probing (BOP) and tooth mobility (TM) before and after implant placement. Besides, we explored the effects of the natural periodontal status on PD, BOP and marginal bone loss (MBL) of the implant at the last follow-up examination by univariate analysis and multivariate analysis. Results: Fifty-three patients were followed up for (44.5±14.1) months in average, with longest interval of (8.3±2.7) months. The PD of adjacent natural teeth in the edentulous area improved from 4.3 (3.6, 4.6) mm before implantation to 3.6 (3.2, 4.0) mm in the last review (P<0.01), while the proportion of BOP (+) improved from 69.6% (94/135) before implantation to 46.7% (63/135) in the last review (P<0.01). The proportion of teeth with mobility≥Ⅱ decreased from 15.6% (21/135) to 5.9% (8/135) (P<0.01). The percentage of natural teeth with PD≥4 mm in the same segment improved from 21.0% (13.3%, 26.0%) before implantation to 18.0% (12.0%, 25.0%) in the last review (P<0.05). The BOP (+)% improved from 29.0% (24.0%, 35.0%) before implantation to 23.0% (18.0%, 31.0%) in the last review (P<0.05), and the number of teeth with mobility≥Ⅱ decreased from 0.0 (0.0, 1.0) to 0.0 (0.0, 0.8) (P<0.05). The functional tooth unit score of full natural teeth increased from 8.0 (6.0, 10.0) points before implantation to 12.0 (12.0, 12.0) points in the last review (P<0.01). PD≥4 mm % increased from 11.0% (6.0%, 25.0%) before implantation to 13.0% (3.0%, 21.0%) in the last review (P<0.05) and there was no significant differences in BOP (+)% [(17.0±9.7) % vs (14.6±7.2) %, P>0.05]. The number of teeth with mobility≥Ⅱ decreased from 1.0 (0.0, 1.8) to 0.0 (0.0, 0.8) (P<0.05). Conclusions: Under the premise of regular supportive care, implant restorative treatment in the posterior region of severe periodontitis patients is helpful to improve the PD, BOP and TM of remaining natural teeth. Besides, the stages and grades of periodontitis at initial diagnosis can affect the PD and BOP of implants.

Segmentation of Bone Surface from Ultrasound Using a Lightweight Network UBS-Net

OBJECTIVE

Ultrasound-assisted orthopaedic navigation holds promise due to its non-ionizing feature, portability, low cost, and real-time performance. To facilitate the applications, it is critical to have accurate and real-time bone surface segmentation. Nevertheless, the imaging artifacts and low signal-to-noise ratios in the tomographical B-mode ultrasound (B US) images-create substantial challenges in bone surface detection. In this study, we present an end-to-end lightweight US bone segmentation network (UBS-Net) for bone surface detection. Approach. We present an end-to-end lightweight UBS-Net for bone surface detection, using the U-Net structure as the base framework and a level set loss function for improved sensitivity to bone surface detectability. A dual attention (DA) mechanism is introduced at the end of the encoder, which considers both position and channel information to obtain the correlation between the position and channel dimensions of the feature map, where axial attention (AA) replaces the traditional self-attention (SA) mechanism in the position attention module for better computational efficiency. The position attention and channel attention (CA) are combined with a two-class fusion module for the DA map. The decoding module finally completes the bone surface detection. Main Results. As a result, a frame rate of 21 frames per second (fps) in detection were achieved. It satisfied the real time requirement. The segmentation quality from the proposed approach outperformed the state-of-the-art method with higher accuracy (Dice similarity coefficient: 88.76% vs. 87.22%) in 612 retrospective testing images. Significance. The proposed UBS-Net for bone surface detection in ultrasound achieved outstanding accuracy and real-time performance. The new method out-performed the state-of-the-art methods. It had potential in US-guided orthopaedic surgery applications. .

Genome-wide profiling of DNA methylome and transcriptome reveals epigenetic regulation of Urechis unicinctus response to sulfide stress

Sulfide is a well-known environmental pollutant that can have detrimental effects on most organisms. However, few metazoans living in sulfide-rich environments have developed mechanisms to tolerate and adapt to sulfide stress. Epigenetic mechanisms, including DNA methylation, have been shown to play a vital role in environmental stress adaptation. Nevertheless, the precise function of DNA methylation in biological sulfide adaptation remains unclear. Urechis unicinctus, a benthic organism inhabiting sulfide-rich intertidal environments, is an ideal model organism for studying adaptation to sulfide environments. In this study, we conducted a comprehensive analysis of the DNA methylome and transcriptome of U. unicinctus after exposure to 50 μM sulfide. The results revealed dynamic changes in the DNA methylation (5-methylcytosine) landscape in response to sulfide stress, with U. unicinctus exhibiting elevated DNA methylation levels following stress exposure. Integrating differentially expressed genes (DEGs) and differentially methylated regions (DMRs), we identified a crucial role of gene body methylation in predicting gene expression. Furthermore, using a DNA methyltransferase inhibitor, we validated the involvement of DNA methylation in the sulfide stress response and the gene regulatory network influenced by DNA methylation. The results indicated that by modulating DNA methylation levels during sulfide stress, the expression of glutathione S-transferase, glutamyl aminopeptidase, and cytochrome c oxidase could be up-regulated, thereby facilitating the metabolism and detoxification of exogenous sulfides. Moreover, DNA methylation was found to regulate and enhance the oxidative phosphorylation pathway, including NADH dehydrogenase, isocitrate dehydrogenase, and ATP synthase. Additionally, DNA methylation influenced the regulation of Cytochrome P450 and macrophage migration inhibitory factor, both of which are closely associated with oxidative stress and stress resistance. Our findings not only emphasize the role of DNA methylation in sulfide adaptation but also provide novel insights into the potential mechanisms through which marine organisms adapt to environmental changes.

A High Precision, Wide Dynamic Range Closed-Loop Neuromodulation IC With Rapid Stimulation Artifact Recovery

This article presents a high precision, wide dynamic range (DR) closed-loop neuromodulation (CLNM) system that can completely reject stimulation artifacts (SA) and achieve rapid SA recovery. In the recorder, a novel SA quick-blanking scheme is proposed for rail-to-rail SA rejection while minimizing SA recovery time. Besides, a new analog front-end (AFE) architecture based on a frequency-shaping (FS) technique is developed to extend DR intrinsically. In the stimulator, a stimulation driver implemented with a proposed redundant crossfire (RXF) technique is incorporated to improve the effective resolution of the stimulation current. The designed CLNM system is implemented in a 180 nm Bipolar-CMOS-DMOS (BCD) process. Measurement results show that the system is capable of tolerating rail-to-rail (5 V) SA and reducing the SA recovery time from 12 ms to 0.15 ms. The FS recorder extends the DR at low frequencies (LF) to 17.5 bits to enhance tolerance to LF interferences. The proposed stimulator adopting the 4-way RXF topology improves the effective resolution to 12.75 bits without consuming much extra area and power. Animal experiments demonstrate that the designed system can acquire high-fidelity neural signals immediately after stimulation onsets, thus supporting concurrent recording and stimulation.

Polymer-Surface-Mediated Mechanochemical Reaction for Rapid and Scalable Manufacture of Perovskite QD Phosphors

Perovskite quantum dots (QDs) have been considered new-generation emitters for lighting and displays due to their high photoluminescence (PL) efficiency, and pure color. However, their commercialization process is currently hindered by the challenge of mass production in a quick and environmentally friendly manner. In this study, a polymer-surface-mediated mechanochemical reaction (PMR) is proposed to prepare perovskite QDs using a high-speed multifunction grinder for the first time. PMR possesses two distinctive features: i) The ultra-high rotating speed (>15 000 rpm) of the grinder facilitates the rapid conversion of the precursor to perovskite; ii) The surface-rich polymer particulate ensures QDs with high dispersity, avoiding QD aggregation-induced PL quenching. Therefore, PMR can successfully manufacture green perovskite QDs with a high PL quantum yield (PLQY) exceeding 90% in a highly material- (100% yield), time- (1 kg min-1), and effort- (solvent-free) efficient manner. Moreover, the PMR demonstrates remarkable versatility, including synthesizing by various polymers and producing diverse colored and Pb-free phosphors. Importantly, these phosphors featuring a combination of polymer and perovskite, are facilely processed into various solid emitters. The proposed rapid, green, and scalable approach has great potential to accelerate the commercialization of perovskite QDs.

KRAS Mutation Detection with (2S,4R)-4-[18F]FGln for Noninvasive PDAC Diagnosis

Pancreatic ductal adenocarcinoma (PDAC), which has a poor prognosis and nonspecific symptoms and progresses rapidly, is the most common pancreatic cancer type. Inhibitors targeting KRAS G12D and G12C mutations have been pivotal in PDAC treatment. Cancer cells with different KRAS mutations exhibit various degrees of glutamine dependency; in particular, cells with KRAS G12D mutations exhibit increased glutamine uptake. (2S,4R)-4-[18F]FGln has recently been developed for clinical cancer diagnosis and tumor cell metabolism analysis. Thus, we verified the heterogeneity of glutamine dependency in PDAC models with different KRAS mutations by a visual and noninvasive method with (2S,4R)-4-[18F]FGln. Two tumor-bearing mouse models (bearing the KRAS G12D or G12C mutation) were injected with (2S,4R)-4-[18F]FGln, and positron emission tomography (PET) imaging features and biodistribution were observed and analyzed. The SUVmax in the regions of interest (ROI) was significantly higher in PANC-1 (G12D) tumors than in MIA PaCa-2 (G12C) tumors. Biodistribution analysis revealed higher tumor accumulation of (2S,4R)-4-[18F]FGln and other metrics, such as T/M and T/B, in the PANC-1 mouse models compared to those in the MIAPaCa-2 mouse models. In conclusion, PDAC cells with the KRAS G12D and G12C mutations exhibit various degrees of (2S,4R)-4-[18F]FGln uptake, indicating that (2S,4R)-4-[18F]FGln might be applied to detect KRAS G12C and G12D mutations and provide treatment guidance.

A single-chain antibody construct with specificity of a natural IgM antibody reduces hepatic ischemia reperfusion injury in mice

Natural immunoglobulin M (IgM) antibodies have been shown to recognize post-ischemic neoepitopes following reperfusion of tissues and to activate complement. Specifically, IgM antibodies and complement have been shown to drive hepatic ischemia reperfusion injury (IRI). Herein, we investigate the therapeutic effect of C2 scFv (single-chain antibody construct with specificity of a natural IgM antibody) on hepatic IRI in C57BL/6 mice. Compared with PBS-treated mice, C2 scFv-treated mice displayed almost no necrotic areas, significant reduction in serum ALT, AST and LDH levels, and significantly reduced in the number of TUNEL positive cells. Moreover, C2 scFv-treated mice exhibited a notable reduction in inflammatory cells after hepatic IRI than PBS-treated mice. The serum IL-6, IL-1β, TNF-α and MPC-1 levels were also severely suppressed by C2 scFv. Interestingly, C2 scFv reconstituted hepatic inflammation and IRI in Rag1-/- mice. We found that C2 scFv promoted hepatic cell death and increased inflammatory cytokines and infiltration of inflammatory cells after hepatic IRI in Rag1-/- mice. In addition, IgM and complement 3d (C3d) were deposited in WT mice and in Rag1-/- mice reconstituted with C2 scFv, indicating that C2 scFv can affect IgM binding and complement activation and reconstitute hepatic IRI. C3d expression was significantly lower in C57BL/6 mice treated with C2 scFv compared to PBS, indicating that excessive exogenous C2 scFv inhibited complement activation. These data suggest that C2 scFv alleviates hepatic IRI by blocking complement activation, and treatment with C2 scFv may be a promising therapy for hepatic IRI.

[177Lu]Lu-labeled anti-claudin-18.2 antibody demonstrated radioimmunotherapy potential in gastric cancer mouse xenograft models

PURPOSE

Gastric cancer (GC), one of the most prevalent and deadliest tumors worldwide, is often diagnosed at an advanced stage with limited treatment options and poor prognosis. The development of a CLDN18.2-targeted radioimmunotherapy probe is a potential treatment option for GC.

METHODS

The CLDN18.2 antibody TST001 (provided by Transcenta) was conjugated with DOTA and radiolabeled with the radioactive nuclide 177Lu. The specificity and targeting ability were evaluated by cell uptake, imaging and biodistribution experiments. In BGC823CLDN18.2/AGSCLDN18.2 mouse models, the efficacy of [177Lu]Lu-TST001 against CLDN18.2-expressing tumors was demonstrated, and toxicity was evaluated by H&E staining and blood sample testing.

RESULTS

[177Lu]Lu-TST001 was labeled with an 99.17%±0.32 radiochemical purity, an 18.50 ± 1.27 MBq/nmol specific activity and a stability of ≥ 94% after 7 days. It exhibited specific and high tumor uptake in CLDN18.2-positive xenografts of GC mouse models. Survival studies in BGC823CLDN18.2 and AGSCLDN18.2 tumor-bearing mouse models indicated that a low dose of 5.55 MBq and a high dose of 11.10 MBq [177Lu]Lu-TST001 significantly inhibited tumor growth compared to the saline control group, with the 11.1 MBq group showing better therapeutic efficacy. Histological staining with hematoxylin and eosin (H&E) and Ki67 immunohistochemistry of residual tissues confirmed tumor tissue destruction and reduced tumor cell proliferation following treatment. H&E showed that there was no significant short-term toxicity observed in the heart, spleen, stomach or other important organs when treated with a high dose of [177Lu]Lu-TST001, and no apparent hematotoxicity or liver toxicity was observed.

CONCLUSION

In preclinical studies, [177Lu]Lu-TST001 demonstrated significant antitumor efficacy with acceptable toxicity. It exhibits strong potential for clinical translation, providing a new promising treatment option for CLDN18.2-overexpressing tumors, including GC.

Nitrogen-Based Gas Molecule Adsorption on a ReSe2 Monolayer via Single-Atom Doping: A First-Principles Study

Two-dimensional materials have shown immense promise for gas-sensing applications due to their remarkable surface-to-volume ratios and tunable chemical properties. However, despite their potential, the utilization of ReSe2 as a gas-sensing material for nitrogen-containing molecules, including NO2, NO, and NH3, has remained unexplored. The choice of doping atoms in ReSe2 plays a pivotal role in enhancing the gas adsorption and gas-sensing capabilities. Herein, the adsorption properties of nitrogen-containing gas molecules on metal and non-metal single-atom (Au, Pt, Ni, P, and S)-doped ReSe2 monolayers have been evaluated systematically via ab initio calculations based on density functional theory. The findings strongly suggest that intrinsic ReSe2 has better selectivity toward NO2 than toward NO and NH3. Moreover, our results provide compelling evidence that all of the dopants, with the exception of S, significantly enhance both the adsorption strength and charge transfer between ReSe2 and the investigated molecules. Notably, P-decorated ReSe2 showed the highest adsorption energy for NO2 and NO (-1.93 and -1.52 eV, respectively) with charge transfer above 0.5e, while Ni-decorated ReSe2 exhibited the highest adsorption energy for NH3 (-0.76 eV). In addition, on the basis of transition theory, we found that only Au-ReSe2 and Ni-ReSe2 can serve as reusable chemiresisitve gas sensors for reliable detection of NO and NH3, respectively. Hence, our findings indicate that gas-sensing applications can be significantly improved by utilizing a single-atom-doped ReSe2 monolayer.

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.

The genetic causal relationship between type 2 diabetes, glycemic traits and venous thromboembolism, deep vein thrombosis, pulmonary embolism: a two-sample Mendelian randomization study

OBJECTIVE

To investigate the genetic underpinnings of the association between type 2 diabetes (T2D), glycemic indicators such as fasting glucose (FG), fasting insulin (FI), and glycated hemoglobin (GH), and venous thromboembolism (VTE), encompassing deep vein thrombosis (DVT) and pulmonary embolism (PE), thereby contributing novel insights to the scholarly discourse within this domain.

METHODS

Genome-wide association study (GWAS) summary data pertaining to exposures (T2D, FG, FI, GH) and outcomes (VTE, DVT, PE) were acquired from the IEU Open GWAS database, encompassing participants of European descent, including both male and female individuals. Two-sample Mendelian randomization (MR) analyses were conducted utilizing the TwoSampleMR and MRPRESSO packages within the R programming environment. The primary analytical approach employed was the random-effects inverse variance weighted (IVW) method. Heterogeneity was assessed via Cochran's Q statistic for MR-IVW and Rucker's Q statistic for MR-Egger. Horizontal pleiotropy was evaluated using the intercept test of MR Egger and MR pleiotropy residual sum and outlier (MR-PRESSO) analysis, with the latter also employed for outlier detection. Additionally, a "Leave one out" analysis was conducted to ascertain the influence of individual single nucleotide polymorphisms (SNPs) on MR results.

RESULTS

The random-effects IVW analysis revealed a negative genetic causal association between T2D) and VTE (P = 0.008, Odds Ratio [OR] 95% confidence interval [CI] = 0.896 [0.827-0.972]), as well as between FG and VTE (P = 0.002, OR 95% CI = 0.655 [0.503-0.853]), GH and VTE (P = 0.010, OR 95% CI = 0.604 [0.412-0.884]), and GH and DVT (P = 0.002, OR 95% CI = 0.413 [0.235-0.725]). Conversely, the random-effects IVW analysis did not detect a genetic causal relationship between FI and VTE (P > 0.05), nor between T2D, FG, or FI and DVT (P > 0.05), or between T2D, FG, FI, or GH and PE (P > 0.05). Both the Cochran's Q statistic for MR-IVW and Rucker's Q statistic for MR-Egger indicated no significant heterogeneity (P > 0.05). Moreover, the intercept tests of MR Egger and MR-PRESSO suggested the absence of horizontal pleiotropy (P > 0.05). MR-PRESSO analysis identified no outliers, while the "Leave one out" analysis underscored that the MR analysis was not influenced by any single SNP.

CONCLUSION

Our investigation revealed that T2D, FG, and GH exhibit negative genetic causal relationships with VTE at the genetic level, while GH demonstrates a negative genetic causal relationship with DVT at the genetic level. These findings furnish genetic-level evidence warranting further examination of VTE, DVT, and PE, thereby making a contribution to the advancement of related research domains.

Study of High-Transverse-Momentum Higgs Boson Production in Association with a Vector Boson in the qqbb Final State with the ATLAS Detector

This Letter presents the first study of Higgs boson production in association with a vector boson (V=W or Z) in the fully hadronic qqbb final state using data recorded by the ATLAS detector at the LHC in proton-proton collisions at sqrt[s]=13  TeV and corresponding to an integrated luminosity of 137  fb^{-1}. The vector bosons and Higgs bosons are each reconstructed as large-radius jets and tagged using jet substructure techniques. Dedicated tagging algorithms exploiting b-tagging properties are used to identify jets consistent with Higgs bosons decaying into bb[over ¯]. Dominant backgrounds from multijet production are determined directly from the data, and a likelihood fit to the jet mass distribution of Higgs boson candidates is used to extract the number of signal events. The VH production cross section is measured inclusively and differentially in several ranges of Higgs boson transverse momentum: 250-450, 450-650, and greater than 650 GeV. The inclusive signal yield relative to the standard model expectation is observed to be μ=1.4_{-0.9}^{+1.0} and the corresponding cross section is 3.1±1.3(stat)_{-1.4}^{+1.8}(syst)  pb.

Clinical-radiomics nomogram for the risk prediction of esophageal fistula in patients with esophageal squamous cell carcinoma treated with intensity-modulated radiation therapy or volumetric-modulated arc therapy

Background

Esophageal fistula (EF) is a serious adverse event as a result of radiotherapy in patients with esophageal cancer (EC). We aimed to identify the predictive factors and establish a prediction model of EF in patients with esophageal squamous cell carcinoma (ESCC) who underwent intensity-modulated radiation therapy (IMRT) or volumetric-modulated arc therapy (VMAT).

Methods

Patients with ESCC treated with IMRT or VMAT from January 2013 to December 2020 at Xijing Hospital were retrospectively analyzed. Ultimately, 43 patients with EF and 129 patients without EF were included in the analysis and propensity-score matched in a 1:3 ratio. The clinical characteristics and radiomics features were extracted. Univariate and multivariate stepwise logistic regression analyses were used to determine the risk factors associated with EF.

Results

The median follow-up time was 24.0 months (range, 1.3-104.9 months), and the median overall survival (OS) was 13.1 months in patients with EF. A total of 1,158 radiomics features were extracted, and eight radiomics features were selected for inclusion into a model for predicting EF, with an area under the receiver operating characteristic curve (AUC) value of 0.794. Multivariate analysis showed that tumor length, tumor volume, T stage, lymphocyte rate (LR), and grade IV esophagus stenosis were related to EF, and the AUC value of clinical model for predicting EF was 0.849. The clinical-radiomics model had the best performance in predicting EF with an AUC value of 0.896.

Conclusions

The clinical-radiomics nomogram can predict the risk of EF in ESCC patients and is helpful for the individualized treatment of EC.

Enhanced Acetone Sensing Properties Based on Au-Pd Decorated ZnO Nanorod Gas Sensor

The mature processes of metal oxide semiconductors (MOS) have attracted considerable interest. However, the low sensitivity of metal oxide semiconductor gas sensors is still challenging, and constrains its practical applications. Bimetallic nanoparticles are of interest owing to their excellent catalytic properties. This excellent feature of bimetallic nanoparticles can solve the problems existing in MOS gas sensors, such as the low response, high operating temperature and slow response time. To enhance acetone sensing performance, we successfully synthesized Au-Pd/ZnO nanorods. In this work, we discovered that Au-Pd nanoparticles modified on ZnO nanorods can remarkably enhance sensor response. The Au-Pd/ZnO gas sensor has long-term stability and an excellent response/recovery process. This excellent sensing performance is attributed to the synergistic catalytic effect of bimetallic AuPd nanoparticles. Moreover, the electronic and chemical sensitization of noble metals also makes a great contribution. This work presents a simple method for preparing Au-Pd/ZnO nanorods and provides a new solution for the detection of acetone based on metal oxide semiconductor.

Noninvasively Deciphering the Immunosuppressive Tumor Microenvironment Using Galectin-1 PET to Inform Immunotherapy Responses

Immune checkpoint blockade (ICB) has achieved groundbreaking results in clinical cancer therapy; however, only a subset of patients experience durable benefits. The aim of this study was to explore strategies for predicting tumor responses to optimize the intervention approach using ICB therapy. Methods: We used a bilateral mouse model for proteomics analysis to identify new imaging biomarkers for tumor responses to ICB therapy. A PET radiotracer was synthesized by radiolabeling the identified biomarker-targeting antibody with 124I. The radiotracer was then tested for PET prediction of tumor responses to ICB therapy. Results: We identified galectin-1 (Gal-1), a member of the carbohydrate-binding lectin family, as a potential negative biomarker for ICB efficacy. We established that Gal-1 inhibition promotes a sensitive immune phenotype within the tumor microenvironment (TME) for ICB therapy. To assess the pre-ICB treatment status of the TME, a Gal-1-targeted PET radiotracer, 124I-αGal-1, was developed. PET imaging with 124I-αGal-1 showed the pretreatment immunosuppressive status of the TME before the initiation of therapy, thus enabling the prediction of ICB resistance in advance. Moreover, the use of hydrogel scaffolds loaded with a Gal-1 inhibitor, thiodigalactoside, demonstrated that a single dose of thiodigalactoside-hydrogel significantly potentiated ICB and adoptive cell transfer immunotherapies by remodeling the immunosuppressive TME. Conclusion: Our study underscores the potential of Gal-1-targeted PET imaging as a valuable strategy for early-stage monitoring of tumor responses to ICB therapy. Additionally, Gal-1 inhibition effectively counteracts the immunosuppressive TME, resulting in enhanced immunotherapy efficacy.

High-nuclearity Luminescent Lanthanide Nanocages for Tumor Drug Delivery

There is an unmet need for easy-to-visualize drug carriers that can deliver therapeutic cargoes deep into solid tumors. Herein, we report the preparation of ultrasmall luminescent imine-based lanthanide nanocages, Eu60 and Tb60 (collectively Ln60 ), designed to encapsulate anticancer chemotherapeutics for tumor therapy. The as-prepared nanocages possess large cavities suitable for the encapsulation of doxorubicin (DOX), yielding DOX@Ln60 nanocages with diameters around 5 nm. DOX@Ln60 are efficiently internalized by breast cancer cells, allowing the cells to be visualized via the intrinsic luminescent property of Ln(III). Once internalized, the acidic intracellular microenvironment promotes imine bond cleavage and the release of the loaded DOX. DOX@Ln60 inhibits DNA replication and triggers tumor cell apoptosis. In a murine triple negative breast cancer (TNBC) model, DOX@Ln60 was found to inhibit tumor growth with negligible side effects on normal tissues. It proved more effective than various controls, including DOX and Ln60 . The present nanocages thus point the way to the development of precise nanomedicines for tumor imaging and therapy.

[A giant malignant melanoma of the palpebral conjunctiva: a case report]

An 81-year-old female patient experienced a rapid increase in the volume of a rice-sized black mass on the left eye over a period of six months. The mass extended out of the eye and exhibited surface erosion with accompanying hemorrhage. Following a live tissue examination and histopathology after orbital exenteration under general anesthesia, the diagnosis of a giant malignant palpebral conjunctival melanoma of the spindle cell subtype was confirmed. The patient refused to undergo local radiation therapy or systemic chemotherapy and died from the disease six months later.

Identification of near-infrared characteristic bands of small bowel necrosis based on cellwise detection algorithm

The near-infrared spectroscopy is often used to distinguish small bowel necrosis due to necrotizing enterocolitis (NEC). The characteristic bands of small bowel necrosis, as an important basis for evaluating the confidence of the differentiation results, are challenging to identify quickly. In this study, we proposed to identify characteristic bands of lesion samples based on hyperspectral imaging (HSI) and cellwise outlier detection. Rabbits were used as an animal model to simulate the clinical symptoms of NEC. The rabbits were detected at intervals of 10, 30, 60, and 90 min. The characteristic bands were identified within the same rabbit, between different rabbits and at different times. The result showed the bands near 763 nm, corresponding to the absorption peak of deoxyhemoglobin, were the characteristic bands separating samples with NEC. The identification result was plausible because hypoxia was the main cause of NEC. The method was easy to perform.

Unveiling the Synergistic Role of Frustrated Lewis Pairs in Carbon-Encapsulated Ni/NiOx Photothermal Cocatalyst for Enhanced Photocatalytic Hydrogen Production

The development of high-density and closely spaced frustrated Lewis pairs (FLPs) is crucial for enhancing catalyst activity and accelerating reaction rates. However, constructing efficient FLPs by breaking classical Lewis bonds poses a significant challenge. Here, this work has made a pivotal discovery regarding the Jahn-Teller effect during the formation of grain boundaries in carbon-encapsulated Ni/NiOx (Ni/NiOx @C). This effect facilitates the formation of high-density O (VO ) and Ni (VNi ) vacancy sites with different charge polarities, specifically FLP-VO -C basic sites and FLP-VNi -C acidic sites. The synergistic interaction between FLP-VO -C and FLP-VNi -C sites not only reduces energy barriers for water adsorption and splitting, but also induces a strong photothermal effect. This mutually reinforcing effect contributes to the exceptional performance of Ni/NiOx @C as a cocatalyst in photothermal-assisted photocatalytic hydrogen production. Notably, the Ni/NiOx @C/g-C3 N4 (NOCC) composite photocatalyst exhibits remarkable hydrogen production activity with a rate of 10.7 mmol g-1 h-1 , surpassing that of the Pt cocatalyst by 1.76 times. Moreover, the NOCC achieves an impressive apparent quantum yield of 40.78% at a wavelength of 380 nm. This work paves the way for designing novel defect-state multiphase cocatalysts with high-density and adjacent FLP sites, which hold promise for enhancing various catalytic reactions.

Research on dynamic characteristics of cutter breaking frozen soil and optimal drum rotation speed of the new shaft tunneling machine

To improve the efficiency of frozen soil excavation, the new shaft tunneling machine was developed. The new shaft tunneling machine exerts pressure on the frozen soil through the cutter under the joint action of its own gravity, the drum rotational force and the inertia force, and the frozen soil is damaged. By unique way of breaking frozen soil to improve the efficiency of frozen soil excavation, the drum rotation speed is one of the factors affecting the performance of frozen soil excavation. This article applies SolidWorks software to establish the model of cutter breaking frozen soil, takes advantage of Hyper Mesh finite element software coupled with LS-DYNA solver to acquire the regular pattern of change in the force change, frozen soil stress-strain and specific energy of cutter crushing frozen soil, etc., which analyzes the destruction of frozen soil when the drum of the new shaft tunneling machine is rotating at the speed of 25-40 rpm. Combine with field test to investigate the mechanism of cutter breaking frozen soil under the optimal drum rotation speed. The investigation results demonstrate that: when frozen soil's self-bearing capacity is lower than the force of cutter, it breaks up and detaches from the soil body, and frozen soil undergoes tensile, compressive and shear damages. For this research, it is instructive for practical engineering.

Measurement of the Centrality Dependence of the Dijet Yield in p+Pb Collisions at sqrt[s_{NN}]=8.16 TeV with the ATLAS Detector

ATLAS measured the centrality dependence of the dijet yield using 165  nb^{-1} of p+Pb data collected at sqrt[s_{NN}]=8.16  TeV in 2016. The event centrality, which reflects the p+Pb impact parameter, is characterized by the total transverse energy registered in the Pb-going side of the forward calorimeter. The central-to-peripheral ratio of the scaled dijet yields, R_{CP}, is evaluated, and the results are presented as a function of variables that reflect the kinematics of the initial hard parton scattering process. The R_{CP} shows a scaling with the Bjorken x of the parton originating from the proton, x_{p}, while no such trend is observed as a function of x_{Pb}. This analysis provides unique input to understanding the role of small proton spatial configurations in p+Pb collisions by covering parton momentum fractions from the valence region down to x_{p}∼10^{-3} and x_{Pb}∼4×10^{-4}.

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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The deubiquitinase BRCC3 increases the stability of ZEB1 and promotes the proliferation and metastasis of triple-negative breast cancer cells

Triple negative breast cancer (TNBC) has a high recurrence rate, metastasis rate and mortality rate. The aim of this study is to identify new targets for the treatment of TNBC. Clinical samples are used for screening deubiquitinating enzymes (DUBs). MDA-MB-231 cells and a TNBC mouse model are used for in vitro and in vivo experiments, respectively. Western blot analysis is used to detect the protein expressions of DUBs, zinc finger E-box binding homeobox 1 (ZEB1), and epithelial-mesenchymal transition (EMT)-related markers. Colony formation and transwell assays are used to detect the proliferation, migration and invasion of TNBC cells. Wound healing assay is used to detect the mobility of TNBC cells. Immunoprecipitation assay is used to detect the interaction between breast cancer susceptibility gene 1/2-containing complex subunit 3 (BRCC3) and ZEB1. ZEB1 ubiquitination levels, protein stability, and protein degradation are also examined. Pathological changes in the lung tissues are detected via HE staining. Our results show a significant positive correlation between the expressions of BRCC3 and ZEB1 in clinical TNBC tissues. Interference with BRCC3 inhibits TNBC cell proliferation, migration, invasion and EMT. BRCC3 interacts with ZEB1 and interferes with BRCC3 to inhibit ZEB1 expression by increasing ZEB1 ubiquitination. Interference with BRCC3 inhibits TNBC cell tumorigenesis and lung metastasis in vivo. In all, this study demonstrates that BRCC3 can increase the stability of ZEB1, upregulate ZEB1 expression, and promote the proliferation, migration, invasion, EMT, and metastasis of TNBC cells, providing a new direction for cancer therapy.

Multi-Functional and Flexible Nano-Silver@MXene Heterostructure-Decorated Graphite Felt for Wearable Thermal Therapy

Wearable heaters with multifunctional performances are urgently required for the future personal health management. However, it is still challengeable to fabricate multifunctional wearable heaters simultaneously with flexibility, air-permeability, Joule heating performance, electromagnetic shielding property, and anti-bacterial ability. Herein, silver nanoparticles (AgNPs)@MXene heterostructure-decorated graphite felts are fabricated by introducing MXene nanosheets onto the graphite felts via a simple dip-coating method and followed by a facile in situ growth approach to grow AgNPs on MXene layers. The obtained AgNPs@MXene heterostructure decorated graphite felts not only maintain the intrinsic flexibility, air-permeability and comfort characteristics of the matrixes, but also present excellent Joule heating performance including wide temperature range (30-128 °C), safe operating conditions (0.9-2.7 V), and rapid thermal response (reaching 128 °C within 100 s at 2.7 V). Besides, the multifunctional graphite felts exhibit excellent electromagnetic shielding effectiveness (53 dB) and outstanding anti-bacterial performances (>95% anti-bacterial rate toward Bacillus subtilis, Escherichia coli and Staphy-lococcus aureus). This work sheds light on a novel avenue to fabricate multifunctional wearable heaters for personal healthcare and personal thermal management.

[The cutoff value of small airway dysfunction in children with bronchial asthma]

Objective: To explore the cutoff value for assessing small airway dysfunction in children with asthma. Methods: A total of 364 asthmatic children aged 5 to 14 years, with normal ventilatory function, followed up at the Asthma Clinic of the Children's Hospital of Capital Institute of Pediatrics from January 2017 to January 2018, were selected as the case group. Concurrently, 403 healthy children of the same age range and without any symptoms in the community were chosen as the control group, and pulmonary function tests were conducted. The values of forced expiratory volume in 1 second (FEV1), forced vital capacity (FVC), forced expiratory flow at 50% of FVC (FEF50), forced expiratory flow at 75% of FVC (FEF75) and maximum mid-expiratory flow (MMEF) were compared between case group and control group. Statistical tests such as t-test, χ2 test, or Mann-Whitney U test were used to analyze the differences between the groups. Receiver operating characteristic (ROC) curves were constructed, and the maximum Youden Index was utilized to determine the optimal cutoff values and thresholds for identifying small airway dysfunction in asthmatic children. Results: This study comprised 364 children in the case group (220 boys and 144 girls) and 403 children in the control group (198 boys and 205 girls). The small airway parameters (FEF50%pred, FEF75%pred, MMEF%pred) in the asthmatic group were significantly lower than in the control group (77% (69%, 91%) vs. 95% (83%, 109%), 67% (54%, 82%) vs. 84% (70%, 102%), 76% (66%, 90%) vs. 97% (86%, 113%), Z=12.03, 11.35, 13.66, all P<0.001). The ROC curve area under the curve for FEF50%pred, FEF75%pred, MMEF%pred was 0.75, 0.74, and 0.79, respectively. Using a cutoff value of 80% for FEF50%pred achieved a sensitivity of 56.9% and specificity of 81.4%. A cutoff value of 74% for FEF75%pred resulted in a sensitivity of 67.3% and specificity of 69.2%. Finally, using a cutoff value of 84% for MMEF%pred achieved a sensitivity of 67.9% and specificity of 77.2%. Conclusion: In the presence of normal ventilatory function, utilizing FEF50<80% predicted or MMEF<84% predicted can accurately serve as criteria for identifying small airway dysfunction in children with controlled asthma.

Pseudo-medical image-guided technology based on 'CBCT-only' mode in esophageal cancer radiotherapy

Purpose To minimize the various errors introduced by image-guided radiotherapy (IGRT) in the application of esophageal cancer treatment, this study proposes a novel technique based on the 'CBCT-only' mode of pseudo-medical image guidance. Methods The framework of this technology consists of two pseudo-medical image synthesis models in the CBCT→CT and the CT→PET direction. The former utilizes a dual-domain parallel deep learning model called AWM-PNet, which incorporates attention waning mechanisms. This model effectively suppresses artifacts in CBCT images in both the sinogram and spatial domains while efficiently capturing important image features and contextual information. The latter leverages tumor location and shape information provided by clinical experts. It introduces a PRAM-GAN model based on a prior region aware mechanism to establish a non-linear mapping relationship between CT and PET image domains.  As a result, it enables the generation of pseudo-PET images that meet the clinical requirements for radiotherapy. Results The NRMSE and multi-scale SSIM (MS-SSIM) were utilized to evaluate the test set, and the results were presented as median values with lower quartile and upper quartile ranges. For the AWM-PNet model, the NRMSE and MS-SSIM values were 0.0218 (0.0143, 0.0255) and 0.9325 (0.9141, 0.9410), respectively. The PRAM-GAN model produced NRMSE and MS-SSIM values of 0.0404 (0.0356, 0.0476) and 0.9154 (0.8971, 0.9294), respectively. Statistical analysis revealed significant differences (p < 0.05) between these models and others. The numerical results of dose metrics, including D98 %, Dmean, and D2 %, validated the accuracy of HU values in the pseudo-CT images synthesized by the AWM-PNet. Furthermore, the Dice coefficient results confirmed statistically significant differences (p < 0.05) in GTV delineation between the pseudo-PET images synthesized using the PRAM-GAN model and other compared methods. Conclusion The AWM-PNet and PRAM-GAN models have the capability to generate accurate pseudo-CT and pseudo-PET images, respectively. The pseudo-image-guided technique based on the 'CBCT-only' mode shows promising prospects for application in esophageal cancer radiotherapy.

IGF2BPs as novel m6A readers: Diverse roles in regulating cancer cell biological functions, hypoxia adaptation, metabolism, and immunosuppressive tumor microenvironment

m6A methylation is the most frequent modification of mRNA in eukaryotes and plays a crucial role in cancer progression by regulating biological functions. Insulin-like growth factor 2 mRNA-binding proteins (IGF2BP) are newly identified m6A 'readers'. They belong to a family of RNA-binding proteins, which bind to the m6A sites on different RNA sequences and stabilize them to promote cancer progression. In this review, we summarize the mechanisms by which different upstream factors regulate IGF2BP in cancer. The current literature analyzed here reveals that the IGF2BP family proteins promote cancer cell proliferation, survival, and chemoresistance, inhibit apoptosis, and are also associated with cancer glycolysis, angiogenesis, and the immune response in the tumor microenvironment. Therefore, with the discovery of their role as 'readers' of m6A and the characteristic re-expression of IGF2BPs in cancers, it is important to elucidate their mechanism of action in the immunosuppressive tumor microenvironment. We also describe in detail the regulatory and interaction network of the IGF2BP family in downstream target RNAs and discuss their potential clinical applications as diagnostic and prognostic markers, as well as recent advances in IGF2BP biology and associated therapeutic value.

Pedicle screw path planning for multi-level vertebral fixation

BACKGROUND

For the spinal internal fixation procedures, connecting rods to the pedicle screws are commonly used in all spinal segments from the cervical to sacral spine. So far, we have only seen single vertebral screw trajectory planning methods in literatures. Joint screw placements in multi-level vertebrae with the constraint of an ipsilateral connecting rod are not considered.

PURPOSE

In this paper, a screw trajectory planning method that considers screw-rod joint system with both multi-level vertebral constraints and individual vertebral safety tolerance are proposed.

METHODS

The proposed method addresses three challenging constraints jointly for multi-level vertebral fixation with pedicle screws. First, a cylindrical screw safe passage model is suggested instead of a unique mathematical optimal trajectory for a single pedicle. Second, the flexible screw cap accessibility model is also included. Third, the connecting rod is modeled to accommodate the spine contour and support the needed gripping capacity. The retrospective clinical data of relative normal shape spines from Beijing Jishuitan hospital were used in the testing. The screw trajectories from the existing methods based on single vertebra and the proposed method based on multi-level vertebrae optimization are calculated and compared.

RESULTS

The results showed that the calculated screw placements by the proposed method can achieve 88% success rate without breaking the pedicle cortex and 100% in clinical class A quality (allow less than 2 mm out of the pedicle cortex) compared to 86.1% and 99.1%, respectively, with the existing methods. Expert evaluation showed that the screw path trajectories and the connecting rod calculated by the new method satisfied the clinical implantation requirements.

CONCLUSIONS

The new screw planning approach that seeks an overall optimization for multi-level vertebral fixation is feasible and more advantageous for clinical use than the single vertebral approaches.

Associations of serum gamma-linolenic acid levels with erythema severity and anxiety/depression status in patients with rosacea

BACKGROUND

The development of rosacea is suggested to be closely associated with lipid metabolism, inflammation, and anxiety/depression. Gamma linolenic acid (GLA) is a key factor participating in lipid metabolism, which is also confirmed to regulate the inflammatory response. However, the associations of serum GLA levels with rosacea severity and psychological status still remain unclear.

OBJECTIVE AND LIMITATIONS OF THE STUDY

The present study aimed to investigate the associations of gamma linolenic acid (GLA), a key factor participating in lipid metabolism and the inflammatory response, with rosacea severity and psychological status. The present study still had some limitations. First, this study is a cross-sectional study and does not provide longitudinal evidence about the relationship between GLA and rosacea; Second, the cohort in this study is also relatively small, and a larger cohort is needed in further investigation to reveal the potential role of lipid metabolism in the pathogenesis of rosacea.

METHODS

A total of 62 rosacea patients were consecutively recruited. Patient's Self-Assessment (PSA) scale and Clinician Erythema Assessment (CEA) as well as 7-item Generalized Anxiety Disorder (GAD-7) and 9-item Patient Health Questionnaire (PHQ-9) were conducted to evaluate the degree of erythema severity and anxiety/depression, respectively. Serum GLA levels were determined by gas chromatography mass.

RESULTS

Lower levels of serum GLA in rosacea patients were observed (p<0.001), and subgroup analysis revealed that patients with higher-level GLA had lower scores of PSA, CEA, GAD-7 and PHQ-9. Moreover, Spearman correlation analysis uncovered that serum GLA levels were negatively associated with PSA, CEA, GAD-7 as well and PHQ-9 scores, respectively. Linear regression model found that serum GLA levels at baseline were a predictive factor for prognosis of clinical outcomes after 1-month conventional treatment.

CONCLUSION

The present study indicates that lower levels of serum GLA in rosacea patients are negatively associated with the degree of erythema and anxiety/depression status.

5 signature genes revealed by single-cell profiling identified unique immune subtypes affecting the prognosis of ovarian cancer

OBJECTIVE

Ovarian cancer (OC) ranks among the most prevalent gynecological malignancies, with surgery, chemotherapy, and immunotherapy constituting primary treatment modalities. However, despite advancements, immunotherapy, particularly immune checkpoint inhibitors, has yielded suboptimal outcomes. The pressing need to identify biomarkers predictive of clinical prognosis underscores our objective. We aim to discern gene signatures and establish prognostic subgroups, specifically in the context of immunotherapy and chemotherapy, guiding clinical decision-making.

MATERIALS AND METHODS

We used the Tumor Immunotherapy Gene Expression Resource (TIGER) and The Cancer Genome Atlas (TCGA) databases to extract signature genes of prognostic significance. Unsupervised consensus clustering was employed to classify patients based on these signature genes. The Tumor Immune Estimation Resource (TIMER) database, along with the R packages "maftools" and "ESTIMATE" facilitated immune infiltration estimation. Gene set variation analysis (GSVA) and Kyoto Encyclopedia of Genes and Genomes (KEGG) enrichment analysis were implemented to probe immune-related cell signaling pathways among distinct subtypes. The Tumor Immune Dysfunction and Exclusion (TIDE) database was used to assess immunotherapy effects, while the R package "OncoPredict" evaluated drug sensitivity differences among subtypes.

RESULTS

We identified five prognostically influential genes in ovarian cancer: IGFBP7, JCHAIN, CCDC80, VSIG4, and MS4A1. Utilizing these signature genes, we categorized TCGA-OV patients into five clusters, each associated with varying clinical prognoses. Notably, 2 clusters exhibited superior prognoses, accompanied by enhanced immune cell infiltration. KEGG enrichment analysis revealed their heightened enrichment in cellular immunity and immune cell interaction pathways. Given the elevated expression levels of multiple immune checkpoint molecules, these clusters may substantially benefit from immune checkpoint inhibitor therapy. Additionally, chemotherapy sensitivity analysis indicated their favorable responses to first or second-line chemotherapy regimens.

CONCLUSIONS

We subclustered ovarian cancer patients by 5 signature genes obtained from the Single-cell RNA sequencing (scRNA-seq) dataset, which demonstrated a good typing effect. Patients in the two molecular subtypes showed better survival, higher immune cell infiltration, and higher drug sensitivity. This meticulous typing may help clinicians to quickly assess the prognosis of patients and the response to immunotherapy and chemotherapy.

Research on dynamic comfort maintenance by measuring lower limb edema and seat pressure during simulated seated sleep in flight

Objectives. Seated sleep during flight can bring significant discomfort to passengers. The objective of this research was to study passengers' dynamic comfort maintenance strategies in lower limb postural shifting during seated sleep in flight. Methods. Studies on seated sleep postures and sitting comfort were conducted. First, 40 participants were recruited to the observational research for collecting typical leg postures during seated sleep. Then, an experiment was conducted with the participants simulating seated sleep in the aircraft seat. The changes in lower limb edema and seat pressure in different postures were measured with a bioelectrical impedance device, near-infrared spectroscopy device and pressure mapping device. Results. Six postures were selected through the observational research. The experiment showed that tissues of the thighs and buttocks suffer alternate higher compression by shifting between the six postures. Lower limb edema is higher when the shanks are forward, while the tissue under the ischial tuberosity suffers higher compression when the shanks are neutral. Conclusion. Six motivations for passengers to shift each sitting posture to achieve dynamic comfort were summarized, which helps obtain alternating rest in different body parts. The suggestion of a leg position adjustment system was also proposed.

Estimation and projection of the burden of hearing loss in China: findings from the Global Burden of Disease Study 2019

OBJECTIVES

The comprehensive description of hearing loss in China and the shifting pattern remain unclear. We conducted the study to estimate the burden of hearing loss in China and project the trends from 2020 to 2034.

STUDY DESIGN AND METHOD

Data on the disease burden of hearing loss were extracted from the Global Burden of Disease Study 2019. Estimated annual percentage changes (EAPCs) were calculated to quantify the trends of the age-standardized rates. Projections of hearing loss burden were made until 2034 using Bayesian age-period-cohort analysis.

RESULTS

In China, prevalent cases of hearing loss increased from 224.4 million in 1990 to 426.5 million in 2019, representing an increase of 90.1 %. The age-standardized prevalence rate of hearing loss ranged from 22,592.8/100,000 in 1990-22,612.4/100,000 in 2019, with an EAPC of 0.003 %, representing a stable trend. Of the category of hearing loss, mild hearing loss accounted for the highest proportion, with 331.4 million people. More than 95 million people had moderate-to-complete hearing loss. Moreover, hearing loss was mostly attributable to age-related and other factors for adults and otitis media for children younger than 10 years. Based on the projection results, there will be 561 million people (40.1 % of the total population) have hearing loss by 2034.

CONCLUSIONS

The prevalent cases of hearing loss in China substantially increased over the last 30 years. Over two in five Chinese people will have hearing loss by 2034, thus suggesting more solutions should be established to reduce the burden of hearing loss.

Construction of prediction model for fetal growth restriction during first trimester in an Asian population

OBJECTIVE

To construct a prediction model for fetal growth restriction (FGR) during the first trimester of pregnancy and evaluate its screening performance.

METHODS

This was a prospective cohort study of singleton pregnancies that underwent routine ultrasound screening at 11 to 13 + 6 weeks at the Affiliated Suzhou Hospital of Nanjing Medical University between January 2019 and April 2022. Basic clinical information, ultrasound indicators and serum biomarkers of pregnant women were collected. Fetal weight assessment was based on the fetal growth curve for the Southern Chinese population. FGR was diagnosed according to Delphi consensus criteria. Least absolute shrinkage and selection operator (lasso) regression was used to select variables for inclusion in the model. Discrimination, calibration and clinical effectiveness of the model were evaluated in training and validation cohorts.

RESULTS

A total of 1188 pregnant women were included, of whom 108 had FGR. Lasso regression identified seven predictive features, including history of maternal hypertension, maternal smoking or passive smoking, gravidity, uterine artery pulsatility index, ductus venosus pulsatility index and multiples of the median values of placental growth factor and soluble fms-like tyrosine kinase-1. The nomogram prediction model constructed from these seven variables accurately predicted FGR, and the area under the receiver-operating-characteristics curve in the validation cohort was 0.82 (95% CI, 0.74-0.90). The calibration curve and Hosmer-Lemeshow test demonstrated good calibration, and the clinical decision curve and clinical impact curve supported its practical value in a clinical setting.

CONCLUSION

The multi-index prediction model for FGR has good predictive value during the first trimester. © 2023 The Authors. Ultrasound in Obstetrics & Gynecology published by John Wiley & Sons Ltd on behalf of International Society of Ultrasound in Obstetrics and Gynecology.

Organic Electrolyte Additive: Dual Functions Toward Fast Sulfur Conversion and Stable Li Deposition for Advanced Li-S Batteries

Lithium-sulfur (Li-S) battery is of great potential for the next generation energy storage device due to the high specific capacity energy density. However, the sluggish kinetics of S redox and the dendrite Li growth are the main challenges to hinder its commercial application. Herein, an organic electrolyte additive, i.e., benzyl chloride (BzCl), is applied as the remedy to address the two issues. In detail, BzCl can split into Bz· radical to react with the polysulfides, forming a Bz-S-Bz intermediate, which changes the conversion path of S and improves the kinetics by accelerating the S splitting. Meanwhile, a tight and robust solid electrolyte interphase (SEI) rich in inorganic ingredients namely LiCl, LiF, and Li2 O, is formed on the surface of Li metal, accelerating the ion conductivity and blocking the decomposition of the solvent and lithium polysulfides. Therefore, the Li-S battery with BzCl as the additive remains high capacity of 693.2 mAh g-1 after 220 cycles at 0.5 C with a low decay rate of 0.11%. This work provides a novel strategy to boost the electrochemical performances in both cathode and anode and gives a guide on the electrolyte design toward high-performance Li-S batteries.

Chemoselective Luche-type reduction of α,β-unsaturated ketones by aluminium hydride catalysis

A novel, simple, eco-friendly, non-toxic aluminium catalyst was synthesised for the chemoselective reduction of α,β-unsaturated ketones. A wide range of ketones were achieved with excellent yields, mild conditions, and low catalyst loading. Furthermore, this unprecedented method allowed for the stereoselective reduction of natural ketones.

Bioinspired Solar-Driven Osmosis for Stable High Flux Desalination

The growing global water crisis necessitates sustainable desalination solutions. Conventional desalination technologies predominantly confront environmental issues such as high emissions from fossil-fuel-driven processes and challenges in managing brine disposal during the operational stages, emphasizing the need for renewable and environmentally friendly alternatives. This study introduces and assesses a bioinspired, solar-driven osmosis desalination device emulating the natural processes of mangroves with effective contaminant rejection and notable productivity. The bioinspired solar-driven osmosis (BISO) device, integrating osmosis membranes, microporous absorbent paper, and nanoporous ceramic membranes, was evaluated under different conditions. We conducted experiments in both controlled and outdoor settings, simulating seawater with a 3.5 wt % NaCl solution. With a water yield of 1.51 kg m-2 h-1 under standard solar conditions (one sun), the BISO system maintained excellent salt removal and accumulation resistance after up to 8 h of experiments and demonstrated great cavitation resistance even at 58.14 °C. The outdoor test recorded a peak rate of 1.22 kg m-2 h-1 and collected 16.5 mL in 8 h, showing its practical application potential. These results highlight the BISO device's capability to address water scarcity using a sustainable approach, combining bioinspired design with solar power, presenting a viable pathway in renewable-energy-driven desalination technology.

Mesoporous and Encapsulated In2O3/Ti3C2Tx Schottky Heterojunctions for Rapid and ppb-Level NO2 Detection at Room Temperature

Rapid and ultrasensitive detection of toxic gases at room temperature is highly desired in health protection but presents grand challenges in the sensing materials reported so far. Here, we present a gas sensor based on novel zero dimensional (0D)/two dimensional (2D) indium oxide (In2O3)/titanium carbide (Ti3C2Tx) Schottky heterostructures with a high surface area and rich oxygen vacancies for parts per billion (ppb) level nitrogen dioxide (NO2) detection at room temperature. The In2O3/Ti3C2Tx gas sensor exhibits a fast response time (4 s), good response (193.45% to 250 ppb NO2), high selectivity, and excellent cycling stability. The rich surface oxygen vacancies play the role of active sites for the adsorption of NO2 molecules, and the Schottky junctions effectively adjust the charge-transfer behavior through the conduction tunnel in the sensing material. Furthermore, In2O3 nanoparticles almost fully cover the Ti3C2Tx nanosheets which can avoid the oxidation of Ti3C2Tx, thus contributing to the good cycling stability of the sensing materials. This work sheds light on the sensing mechanism of heterojunction nanostructures and provides an efficient pathway to construct high-performance gas sensors through the rational design of active sites.

In ovo injection of AZD6244 suppresses feather follicle development by the inhibition of ERK and Wnt/β-catenin pathways in goose embryos (Anser cygnoides)

1. Feathers are an important product from poultry, and the state of feather growth and development plays an important role in their economic value.2. In total, 120 eggs were selected for immunoblotting and immunolocalisation experiments of ERK and β-catenin proteins in different developmental stages of goose embryos. The ERK protein was highly expressed in the early stage of goose embryo development, while β-catenin protein was highly expressed in the middle stage of embryo development.3. The 120 eggs were divided into four treatment groups, including an uninjected group (BLANK), a group injected with 100 µl of cosolvent (CK), a group injected with 100 µl of AZD6244 containing cosolvent in a dose of 5 mg/kg AZD6244 containing cosolvent (AZD5) and a group injected with 100 µl of AZD6244 containing cosolvent in a dose of 15 mg/kg AZD6244 containing cosolvent (AZD15). The eggs were injected on the ninth day of embryonic development (E9). Samples were collected at E21.5 to observe feather width, feather follicle diameter, ERK and Wnt/β-catenin pathway protein expression.4. The AZD5 and AZD15 doses were within the embryonic safety range compared to the BLANK and CK groups and had no significant effect on the survival rate and weight at the inflection point, but significantly reduced the feather width and feather follicle diameter (p < 0.05). The AZD6244 treatment inhibited ERK protein phosphorylation levels and blocked the Wnt/β-catenin pathway, which in turn significantly down-regulated the expression levels of FZD4, β-catenin, TCF4 and LEF1 (p < 0.05), with an inhibitory effect in the AZD15 group being more significant. The immunohistochemical results of β-catenin and p-ERK were consistent with Western blot results.5. The small molecule inhibitor AZD6244 regulated the growth and development of feather follicles in goose embryos by the ERK and Wnt/β-catenin pathways.

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.

Search for New Phenomena in Two-Body Invariant Mass Distributions Using Unsupervised Machine Learning for Anomaly Detection at sqrt[s]=13 TeV with the ATLAS Detector

Searches for new resonances are performed using an unsupervised anomaly-detection technique. Events with at least one electron or muon are selected from 140  fb^{-1} of pp collisions at sqrt[s]=13  TeV recorded by ATLAS at the Large Hadron Collider. The approach involves training an autoencoder on data, and subsequently defining anomalous regions based on the reconstruction loss of the decoder. Studies focus on nine invariant mass spectra that contain pairs of objects consisting of one light jet or b jet and either one lepton (e,μ), photon, or second light jet or b jet in the anomalous regions. No significant deviations from the background hypotheses are observed. Limits on contributions from generic Gaussian signals with various widths of the resonance mass are obtained for nine invariant masses in the anomalous regions.

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.

Electrical-Driven Directed-Evolution of Copper Nanowires Catalysts for Efficient Nitrate Reduction to Ammonia

The electrocatalytic conversion of nitrate (NO3 - ) to NH3 (NO3 RR) at ambient conditions offers a promising alternative to the Haber-Bosch process. The pivotal factors in optimizing the proficient conversion of NO3 - into NH3 include enhancing the adsorption capabilities of the intermediates on the catalyst surface and expediting the hydrogenation steps. Herein, the Cu/Cu2 O/Pi NWs catalyst is designed based on the directed-evolution strategy to achieve an efficient reduction of NO3 ‾. Benefiting from the synergistic effect of the OV -enriched Cu2 O phase developed during the directed-evolution process and the pristine Cu phase, the catalyst exhibits improved adsorption performance for diverse NO3 RR intermediates. Additionally, the phosphate group anchored on the catalyst's surface during the directed-evolution process facilitates water electrolysis, thereby generating Hads on the catalyst surface and promoting the hydrogenation step of NO3 RR. As a result, the Cu/Cu2 O/Pi NWs catalyst shows an excellent FE for NH3 (96.6%) and super-high NH3 yield rate of 1.2 mol h-1  gcat. -1 in 1 m KOH and 0.1 m KNO3 solution at -0.5 V versus RHE. Moreover, the catalyst's stability is enhanced by the stabilizing influence of the phosphate group on the Cu2 O phase. This work highlights the promise of a directed-evolution approach in designing catalysts for NO3 RR.

The Causal Association Between Blood Lead and Sleep Disorders: Evidence from National Health and Nutrition Examination Survey and Mendelian Randomization Analysis

BACKGROUND

Poor sleep quality is a global public health concern. This study aimed to identify the risk factors for sleep disorders and clarify their causal effects.

METHODS

Data were obtained from the National Health and Nutrition Examination Survey (NHANES) and Mendelian randomization (MR)-Base databases. Baseline characteristics of individuals with and without sleep disorders were compared. A multivariate logistic regression analysis was performed to calculate the effects of each variable on sleep disorders. Causal effects of blood lead levels and hypertension on sleep disorders were assessed using MR analysis.

RESULTS

In total, 3660 individuals were enrolled in the study. The prevalence of self-reported sleep disorders was 26.21%. Serum lead level, serum mercury level, serum retinol level, prevalence of hypertension, and daily vigorous work duration were significantly higher for those in the sleep disorders group than the control group. After adjusting for various covariates, the effects of serum lead and hypertension on sleep disorders were stable from logistic regression models 1-4. MR analysis showed that blood lead levels were causally related to the risk of sleep disorders (odds ratio (OR) = 1.09, 95% confidence interval (CI) 1.01-1.17, P = 0.030). There was no causal link between elevated blood pressure and sleep disorders (OR = 0.99, 95% CI 0.94-1.04, P = 0.757). Goodness-of-fit tests and sensitivity analyses were used to verify the reliability of the results.

CONCLUSIONS

Blood lead is positively and causally associated with an increased risk of sleep disorders. These findings provide a novel perspective regarding sleep protection. Taking effective measures to reduce lead exposure may significantly improve sleep health.