Influencing factors of clinical efficacy of roxadustat among hemodialysis patients

OBJECTIVE

To explore independent influencing factors for clinical efficacy of roxadustat in hemodialysis patients.

METHODS

Hemodialysis patients treated with roxadustat were enrolled. The plasma trough concentrations of roxadustat were measured using liquid chromatography-tandem mass spectrometry (LC-MS/MS). A multiple logistic regression model was established to determine the factors that affect clinical efficacy of roxadustat in patients undergoing hemodialysis.

RESULTS

A total of 67 hemodialysis patients were enrolled in the study. The results showed that age, blood trough concentration of roxadustat, and baseline hemoglobin (Hb) level were independent factors of clinical efficacy of roxadustat (OR = 1.06, p = .025 for age; OR = 1.001, p = .037 for plasma concentration; and OR = 0.941, p = .003 for baseline Hb), with an AUC score of 0.859.

CONCLUSIONS

Age, blood trough concentration of roxadustat, and baseline Hb level were independent influencing factors of the response to roxadustat in hemodialysis patients.

High ambient temperature may increase the risk of anemia in pregnancy: Identifying susceptible exposure windows

Anemia in pregnancy (AIP) is associated with multiple severe maternal and perinatal adverse outcomes. However, there is a lack of evidence on the association between environmental factors and AIP. Aim to explore the association between ambient temperature and the risk of AIP, and identify susceptible exposure windows, we conducted a matched case-control study from 2013 to 2016 in Xi'an, China, which included 710 women with AIP and 1420 women without AIP. The conditional logistic regression model was used to evaluate the association between ambient temperature and AIP at different gestational weeks and gestational months. The association between extreme temperature and AIP was evaluated using the distributed lag nonlinear model (DLNM). We conducted stratified analyses of age, parity, and season of conception, and estimated the interaction between ambient temperature and air pollutants on AIP. Ambient temperature was significantly positively associated with the risk of AIP, and the susceptible exposure windows were 2-25 gestational weeks and 1-6 gestational months, respectively. The strongest effect was observed in the week 8 and month 2, for each 1 °C increase in weekly and monthly mean temperature, the odds ratio (OR) for AIP was 1.038 (95 % confidence interval (CI): 1.022, 1.055) and 1.040 (95 % CI: 1.020, 1.060), respectively. Extreme heat may increase the risk of AIP. Stratified analyses showed that there was no significant difference among different age, parity, and season of conception groups. No significant interaction effect of ambient temperature with air pollution on AIP was found. In summary, high ambient temperature may increase the risk of AIP, and the first and second trimesters may be susceptible exposure windows. Understanding the effect of temperature on pregnant women will be beneficial to reduce the occurrence of AIP.

Genomic Landscape of Lynch Syndrome Colorectal Neoplasia Identifies Shared Mutated Neoantigens for Immunoprevention

BACKGROUND & AIMS

Lynch syndrome (LS) carriers develop mismatch repair-deficient neoplasia with high neoantigen (neoAg) rates. No detailed information on targetable neoAgs from LS precancers exists, which is crucial for vaccine development and immune-interception strategies. We report a focused somatic mutation and frameshift-neoAg landscape of microsatellite loci from colorectal polyps without malignant potential (PWOMP), precancers, and early-stage cancers in LS carriers.

METHODS

We generated paired whole-exome and transcriptomic sequencing data from 8 colorectal PWOMP, 41 precancers, 8 advanced precancers, and 12 early-stage cancers of 43 LS carriers. A computational pipeline was developed to predict, rank, and prioritize the top 100 detected mutated neoAgs that were validated in vitro using ELISpot and tetramer assays.

RESULTS

Mutation calling revealed >10 mut/Mb in 83% of cancers, 63% of advanced precancers, and 20% of precancers. Cancers displayed an average of 616 MHC-I neoAgs/sample, 294 in advanced precancers, and 107 in precancers. No neoAgs were detected in PWOMP. A total of 65% of our top 100 predicted neoAgs were immunogenic in vitro, and were present in 92% of cancers, 50% of advanced precancers, and 29% of precancers. We observed increased levels of naïve CD8+ and memory CD4+ T cells in mismatch repair-deficient cancers and precancers via transcriptomics analysis.

CONCLUSIONS

Shared frameshift-neoAgs are generated within unstable microsatellite loci at initial stages of LS carcinogenesis and can induce T-cell responses, generating opportunities for vaccine development, targeting LS precancers and early-stage cancers.

[Cloning and functional analysis of AcFMO from onion during alliine biosynthesis]

Flavin-containing monooxygenase (FMO) is the key enzyme in the biosynthesis pathway of CSOs with sulfur oxidation. In order to explore the molecular regulatory mechanism of FMO in the synthesis of onion CSOs, based on transcriptome database and phylogenetic analysis, one AcFMO gene that may be involved in alliin synthesis was obtained, the AcFMO had a cDNA of 1 374 bp and encoded 457 amino acids, which was evolutionarily closest to the AsFMO of garlic. Real-time fluorescence quantitative polymerase chain reaction (qRT-PCR) indicated that AcFMO was the highest in the flowers and the lowest in the leaf sheaths. The results of subcellular localization showed that the AcFMO gene product was widely distributed throughout the cell A yeast expression vector was constructed, and the AcFMO gene was ecotopically overexpressed in yeast to further study the enzyme function in vitro and could catalyze the synthesis of alliin by S-allyl-l-cysteine. In summary, the cloning and functional identification of AcFMO have important reference value for understanding the biosynthesis of CSOs in onions.

Risk factors of neonatal stroke from different origins: a systematic review and meta-analysis

Given the persistent ambiguity regarding the etiology of neonatal stroke across diverse origins, our objective was to conduct a comprehensive evaluation of both qualitative and quantitative risk factors. An exhaustive search of eight databases was executed to amass all pertinent observational studies concerning risk factors for neonatal stroke from various origins. Subsequent to independent screening, data extraction, and bias assessment by two researchers, a meta-analysis was conducted utilizing RevMan and Stata software. Nineteen studies, encompassing a total of 30 factors, were incorporated into this analysis. Beyond established risk factors, our investigation unveiled gestational diabetes (OR, 5.51; P < 0.00001), a history of infertility (OR, 2.44; P < 0.05), placenta previa (OR, 3.92; P = 0.02), postdates (OR, 2.07; P = 0.01), preterm labor (OR, 2.32; P < 0.00001), premature rupture of membranes (OR, 3.02; P = 0.007), a prolonged second stage of labor (OR, 3.94; P < 0.00001), and chorioamnionitis (OR, 4.35; P < 0.00001) as potential risk factors for neonatal cerebral arterial ischemic stroke. Additionally, postdates (OR, 4.31; P = 0.003), preterm labor (OR, 1.60; P < 0.00001), an abnormal CTG tracing (OR, 9.32; P < 0.0001), cesarean section (OR, 4.29; P = 0.0004), male gender (OR, 1.73; P = 0.02), and vaginal delivery (OR, 1.39; P < 0.00001) were associated with an elevated risk for neonatal hemorrhagic stroke.

CONCLUSIONS

This study provides a succinct overview and comparative analysis of maternal, perinatal, and additional risk factors associated with neonatal cerebral artery ischemic stroke and neonatal hemorrhagic stroke, furnishing critical insights for healthcare practitioners involved in the diagnosis and prevention of neonatal stroke. This research also broadens the conceptual framework for future investigations.

WHAT IS KNOWN

• Research indicates that prenatal, perinatal, and neonatal risk factors can elevate the risk of neonatal arterial ischemic stroke (NAIS). However, the risk factors for neonatal cerebral arterial ischemic stroke remain contentious, and those for neonatal hemorrhagic stroke (NHS) and neonatal cerebral venous sinus thrombosis (CVST) are still not well-defined.

WHAT IS NEW

• This study is the inaugural comprehensive review and meta-analysis encompassing 19 studies that explore maternal, perinatal, and various risk factors linked to neonatal stroke of differing etiologies. Notably, our analysis elucidates eight risk factors associated with NAIS: gestational diabetes mellitus, a history of infertility, placenta previa, postdates, preterm birth, premature rupture of membranes, a prolonged second stage of labor, and chorioamnionitis. Furthermore, we identify six risk factors correlated with NHS: postdates, preterm birth, an abnormal CTG, the method of delivery, male gender, and vaginal delivery. Additionally, our systematic review delineates risk factors associated with CVST.

Durable Effects of Acupuncture for Knee Osteoarthritis: A Systematic Review and Meta-analysis

PURPOSE OF REVIEW

Knee osteoarthritis (KOA) is a degenerative joint disease which can result in chronic pain and disability. The current interventions available for KOA often fail to provide long-lasting effects, highlighting the need for new treatment options that can offer durable benefits. Previous studies have suggested the efficacy of acupuncture for knee osteoarthritis (KOA) with its durability remaining uncertain. In this review, we aimed to investigate the durability of the efficacy after completion of treatment.

RECENT FINDINGS

We performed thorough searches of PubMed, EMBASE, Web of Science, and Cochrane Central Register of Controlled Trials from inception to November 4, 2023. The outcomes were assessed at all available time points after completion of treatment. Primary outcomes were changes from baseline in pain and function measured using the Western Ontario and McMaster Universities Osteoarthritis Index (WOMAC) pain and function subscales. Secondary outcomes included response rate, overall pain, the WOMAC stiffness subscale, total WOMAC index, and physical and mental health components of 12/36-item Short-Form Health Survey. A total of 10 randomized controlled trials (RCTs) involving 3221 participants were included. Pooled estimates suggested that acupuncture may offer potential improvements in function and overall pain for 4.5 months post-treatment versus sham acupuncture (SA). Acupuncture may provide durable clinically important pain relief and functional improvement up to 5 months post-treatment versus usual care, and up to 6 months post-treatment versus diclofenac. For acupuncture versus no treatment, one trial with large sample size indicated that improvements in pain and function persisted for 3 months post-treatment, while the other trial reported that significant pain reduction and functional improvement were only observed at the end of the treatment, not at 9 months post-treatment. However, acupuncture as adjunct to exercise-based physical therapy (EPT) showed no superiority to SA as an adjunct to EPT or EPT alone up to 11.25 months after completion of treatment. Acupuncture may provide pain alleviation and functional improvements in KOA patients for 3 to 6 months after completion of treatment with a good safety profile.

Reconstructing dynamics correlation network to simultaneously improve activity and stability of 2,3-butanediol dehydrogenase by design of distal interchain disulfide bonds

The complete enzyme catalytic cycle includes substrate binding, chemical reaction and product release, in which different dynamic conformations are adopted. Due to the complex relationship among enzyme activity, stability and dynamics, the directed evolution of enzymes for improved activity or stability commonly leads to a trade-off in stability or activity. It hence remains a challenge to engineer an enzyme to have both enhanced activity and stability. Here, we have attempted to reconstruct the dynamics correlation network involved with active center to improve both activity and stability of a 2,3-butanediol dehydrogenase (2,3-BDH) by introducing inter-chain disulfide bonds. A computational strategy was first applied to evaluate the effect of introducing inter-chain disulfide bond on activity and stability of three 2,3-BDHs, and the N258C mutation of 2,3-BDH from Corynebacterium glutamicum (CgBDH) was proved to be effective in improving both activity and stability. In the results, CgBDH-N258C showed a different unfolding curve from the wild type, with two melting temperatures (Tm) of 68.3 °C and 50.8 °C, 19.7 °C and 2 °C higher than 48.6 °C of the wild type. Its half-life was also improved by 14.8-fold compared to the wild type. Catalytic efficiency (kcat/Km) of the mutant was increased by 7.9-fold toward native substrate diacetyl and 8.8-fold toward non-native substrate 2,5-hexanedione compared to the wild type. Molecular dynamics simulations revealed that an interaction network formed by Cys258, Arg162, Ala144 and the catalytic residues was reconstructed in the mutant and the dynamics change caused by the disulfide bond could be propagated through the interactions network. This improved the enzyme stability and activity by decreasing the flexibility and locking more "reactive" pose, respectively. Further construction of mutations including A144G showing a 44-fold improvement in catalytic efficiency toward meso-2,3-BD confirmed the role of modifying dynamics correlation network in tunning enzyme activity and selectivity. This study provided important insights into the relationship among dynamics, enzyme catalysis and stability, and will be useful in the designing new enzymes with co-evolution of stability, activity and selectivity.

Adversarially robust neural networks with feature uncertainty learning and label embedding

Deep neural networks (DNNs) are vulnerable to the attacks of adversarial examples, which bring serious security risks to the learning systems. In this paper, we propose a new defense method to improve the adversarial robustness of DNNs based on stochastic neural networks (SNNs), termed as Margin-SNN. The proposed Margin-SNN mainly includes two modules, i.e., feature uncertainty learning module and label embedding module. The first module introduces uncertainty to the latent feature space by giving each sample a distributional representation rather than a fixed point representation, and leverages the advantages of variational information bottleneck method in achieving good intra-class compactness in latent space. The second module develops a label embedding mechanism to take advantage of the semantic information underlying the labels, which maps the labels into the same latent space with the features, in order to capture the similarity between sample and its class centroid, where a penalty term is equipped to elegantly enlarge the margin between different classes for better inter-class separability. Since no adversarial information is introduced, the proposed model can be learned in standard training to improve adversarial robustness, which is much more efficient than adversarial training. Extensive experiments on data sets MNIST, FASHION MNIST, CIFAR10, CIFAR100 and SVHN demonstrate superior defensive ability of the proposed method. Our code is available at https://github.com/humeng24/Margin-SNN.

TGFβ1 Stimulates the Proliferation of Quiescent Oogonial Stem Cells in Chicken

Oogonial stem cells (OSCs) are a type of germ stem cell present in the adult ovary. They have the ability to self-renew through mitosis and differentiate into oocytes through meiosis. We have previously identified a population of OSCs in chicken ovary, but the underlying mechanism control their activation and proliferation were unclear. In this study, we observed that OSCs showed robust proliferation when cultured on a layer of chicken embryo fibroblasts (CEF), suggesting that CEF may secrete certain crucial factors that activate OSC proliferation. We further detected Transforming Growth Factor beta 1 (TGF-β1) as a potent signaling molecule to promote OSC proliferation. Additionally, we revealed the signaling pathways that play important roles in the downstream of TGF-β1-induced OSC proliferation. These findings provide insights into the mechanisms underlying OSC proliferation in chickens and offer a foundation for future research on in situ activation of OSC proliferation in ovary and improvement of egg-laying performance in chickens.

[Investigation of the population diversity of intermediate host snails and crabs of Paragonimus along Jiulong River, Zhangjiang River and Dongxi River basins in southern Fujian Province]

OBJECTIVE

To investigate the population distribution of intermediate host snails and crabs of Paragonimus along the Jiulongjiang River, Zhangjiang River, and Dongxi River basins in Bopingling Mountain, southern Fujian Province, so as to provide baseline data for researches on parasitic disease prevention and control and enlargement of samples in the parasitic resource bank.

METHODS

A total of 23 villages in 8 counties (districts) along the Jiulong River, Zhangjiang River, and Dongxi River basins in Zhangzhou City, Fujian Province were selected as survey sites during the period from November 2020 through March 2023, and snail and freshwater crabs were sampled from 1 to 3 streams and ditches neighboring residential areas in each village. Morphological identification of snails was performed according to the external morphological characteristics of collected snail shells, and the unidentified snail species sampled from the natural foci of paragonimiasis in Yunxiao County were subjected to se-quence analysis of the mitochondrial cytochrome oxidase 1 (CO1) gene. The crab species was identified by observing the morphological characteristics of the terminal segment of the first pleopod of male crabs, and Paragonimus cercariae and metacercariae were detected in collected snails.

RESULTS

The shells of the unidentified snails sampled from the natural foci of paragonimiasis in Yunxiao County were approximately 50 mm in height and 18 mm in width, thick and solid, long tower cone-shaped, and had 8 to 10 whorls. CO1 gene sequence analysis identified the snail species as Sulcospira hainanensis. A total of 6 freshwater snail species belonging to 5 genera within 3 families, identified 23 survey sites, including Semisulcospira libertina, Paludomus zhangchouensis and S. hainanensis that belonged to the Family Pleurceridae, Tricula fujianensis and T. huaanensis that belonged to the subfamily Triculinae, Family Pomatiopsidae, and Melanoides tuberculata (Family Thiaridae), and 11 species of freshwater crabs belonging to 5 genera within 2 families were identified, including Sinopotamon genus of S. jianglense, S. pinheense, and S. zhangzhouense, Huananpotamon genus of H. planopodum and H. zhangzhouense, Nanhaipotamon genus of N. huaanense and N. longhaiense, and Minpotamon genus of M. nasicum and M. auritum that belonged to the Family Potamidae, and Somanniathelphusa genus of S. huaanensis and S. zhangpuensis (Family Parathelphusidae). In addition, the prevalence of P. westermani cercariae infections was 0.08% (2/2 317) in P. zhangchouensis from Danyan Village in Changtai District and 0.09% (1/1 039) in S. hainanensis from Jinkeng Village in Yunxiao County, and the prevalence of P. westermani metacercariae infections was 25.81% (8/31) in S. jianglense from Danyan Village in Changtai District, and 26.31% (5/19) in S. zhangzhouense from Jinkeng Village in Yunxiao County, respectively.

CONCLUSIONS

There is a population diversity in the intermediate host snails and crabs along the Jiulongjiang River, Zhangjiang River, and Dongxi River basins in Bopingling Mountain, southern Fujian Province, and P. zhangzhouensis and S. hainanensis are, for the first time, confirmed as the first intermediate hosts of P. westermani.

CircALMS1 Alleviates Pulmonary Microvascular Endothelial Cell Dysfunction in Pulmonary Hypertension

BACKGROUND

Circular RNAs can serve as regulators influencing the development of pulmonary hypertension (PH). However, their function in pulmonary vascular intimal injury remains undefined. Thus, we aimed to identify specifically expressed circular RNAs in pulmonary microvascular endothelial cells (PMECs) under hypoxia and PH.

METHODS AND RESULTS

Deep RNA sequencing and quantitative real-time polymerase chain reaction revealed that circALMS1 (circular RNA Alstrom syndrome protein 1) was reduced in human PMECs under hypoxia (P<0.0001). Molecular biology and histopathology experiments were used to elucidate the roles of circALMS1 in regulating PMEC dysfunction among patients with PH. The circALMS1 expression was decreased in the plasma of patients with PH (P=0.0315). Patients with lower circALMS1 levels had higher risk of death (P=0.0006). Moreover, the circALMS1 overexpression of adeno-associated viruses improved right ventricular function and reduced pulmonary vascular remodeling in monocrotaline-PH and sugen/hypoxia-PH rats (P<0.05). Furthermore, circALMS1 overexpression promoted apoptosis and inhibited PMEC proliferation and migration under hypoxia by directly downregulating miR-17-3p (P<0.05). Dual luciferase assay confirmed the direct binding of circALMS1 to miR-17-3p and miR-17-3p binding to its target gene YT521-B homology domain-containing family protein 2 (YTHDF2) (P<0.05). The YTHDF2 levels were also downregulated in hypoxic PMECs (P<0.01). The small interfering RNA YTHDF2 reversed the effects of miR-17-3p inhibitors on PMEC proliferation, migration, and apoptosis. Finally, the results indicated that, although YTHDF2, as an N(6)-methyladenosine reader protein, contributes to the degradation of many circular RNAs, it could not regulate the circALMS1 levels in PMECs (P=0.9721).

CONCLUSIONS

Our study sheds new light on circALMS1-regulated dysfunction of PMECs by the miR-17-3p/YTHDF2 pathway under hypoxia and provides insights into the underlying pathogenesis of PH.

Single-crystal growth, structure and thermal transport properties of the metallic antiferromagnet Zintl-phase β-EuIn2As2

Zintl-phase materials have attracted significant research interest owing to the interplay of magnetism and strong spin-orbit coupling, providing a prominent material platform for axion electrodynamics. Here, we report the single-crystal growth, structure, magnetic and electrical/thermal transport properties of the antiferromagnet layer Zintl-phase compound β-EuIn2As2. Importantly, the new layered structure of β-EuIn2As2, in rhombohedral (R3̄m) symmetry, contains triangular layers of Eu2+ ions. The in-plane resistivity ρ(H, T) measurements reveal metal behavior with an antiferromagnetic (AFM) transition (TN ∼ 23.5 K), which is consistent with the heat capacity Cp(H, T) and magnetic susceptibility χ(H, T) measurements. Negative MR was observed in the temperature range from 2 K to 20 K with a maximum MR ratio of 0.06. Unique 4f7J = S = 7/2 Eu2+ spins were supposed magnetically order along the c-axis. The Seebeck coefficient shows a maximum thermopower |Smax| of about 40 μV K-1. The kink around 23 K in the Seebeck coefficient originates from the effect of the antiferromagnetic phase on the electron band structure, while the pronounced thermal conductivity peak at around 10 K is attributed to the phonon-phonon Umklapp scattering. The results suggest that the Eu2+ spin arrangement plays an important role in the magnetic, electrical, and thermal transport properties in β-EuIn2As2, which might be helpful for future potential technical applications.

Imaging the Meissner effect in hydride superconductors using quantum sensors

By directly altering microscopic interactions, pressure provides a powerful tuning knob for the exploration of condensed phases and geophysical phenomena1. The megabar regime represents an interesting frontier, in which recent discoveries include high-temperature superconductors, as well as structural and valence phase transitions2-6. However, at such high pressures, many conventional measurement techniques fail. Here we demonstrate the ability to perform local magnetometry inside a diamond anvil cell with sub-micron spatial resolution at megabar pressures. Our approach uses a shallow layer of nitrogen-vacancy colour centres implanted directly within the anvil7-9; crucially, we choose a crystal cut compatible with the intrinsic symmetries of the nitrogen-vacancy centre to enable functionality at megabar pressures. We apply our technique to characterize a recently discovered hydride superconductor, CeH9 (ref. 10). By performing simultaneous magnetometry and electrical transport measurements, we observe the dual signatures of superconductivity: diamagnetism characteristic of the Meissner effect and a sharp drop of the resistance to near zero. By locally mapping both the diamagnetic response and flux trapping, we directly image the geometry of superconducting regions, showing marked inhomogeneities at the micron scale. Our work brings quantum sensing to the megabar frontier and enables the closed-loop optimization of superhydride materials synthesis.

The ability of a portable near infrared instrument to evaluate the shelf-life of fresh and thawed goat muscles

The objective of this study was to evaluate the use of a portable near infrared (NIR) instrument to monitor the shelf-life of four goat muscles [longissimus thoracis et lumborum (LTL), semimembranosus (SM), semitendinosus (ST) and biceps femoris (BF)] stored for up to 8 days (4 °C). The NIR spectra of the muscle samples were collected at day 0, and after 1, 4 and 8 days of storage using a MicroNIR instrument (900-1600 nm). The coefficient of determination in cross-validation (R2) and the standard error in cross validation (SECV) obtained for the prediction of days of storage ranged between 0.76 and 0.86, where the SECV ranged from 0.32 to 0.41. The best statistics in cross-validation were obtained for the prediction of days of storage in the BF samples, followed by the ST and LTL muscles. Differences in the PLS loadings for the cross-validation models were observed due to the interactions between the different muscle samples and days of storage. Overall, these results showed the potential of NIR spectroscopy to identify the time of storage in four different goat muscles. Similar data and techniques could be used to predict the remaining shelf life of meat derived from different species under storage. This information can then be used as a tool to predict and guarantee the safety of meat samples to the consumer along the meat supply and value chains.

Impact on early outcome after endovascular repair of type B dissection without proximal landing zone using Castor single-branched stent graft-a retrospective cohort study

Background

The early safety and efficacy of Castor branch stents have been demonstrated. However, the effect of aortic arch morphology on endovascular therapy remains an unresolved issue. This study aims to assess the impact of aortic arch morphology on the early outcomes of endovascular repair using Castor stent graft in patients who have acute type B aortic dissection involving the left subclavian artery (LSA).

Methods

This is a retrospective cohort study. From January 2019 to December 2021, forty-one patients scheduled for thoracic endovascular aortic repair (TEVAR) of TBADs from Beijing Anzhen Hospital were enrolled in this retrospective cohort study and divided into two groups based on the length of the proximal landing zone left common carotid artery-LSA (PLZ LCCA-LSA), specifically the distance between the LCCA and the LSA (group A ≤10 mm and group B >10 mm). The study recorded technical success, mortality and aortic-related post-operative adverse events. Morphological indices were analyzed including the bird-beak configuration. The bird-beak configuration refers to the wedge-shaped gap between the undersurface of the endograft and the lesser curvature of the arch. The relationship between the risk of bird-beak configuration and PLZ was assessed with logistic regression analysis. Meanwhile, the relationship between the risk of aortic-related adverse events and bird-beak configuration was assessed with logistic regression analysis. Follow-up data were analyzed by Kaplan-Meier life table analysis.

Results

The study included 41 patients with a mean age of 63.1±9.2 years, of which 80.5% were male. 18 patients from group A and 23 patients from group B were included in the comparative analysis. There were no significant differences in aortic-related adverse events, bird-beak phenomenon and re-intervention between groups A and B in 30-day outcomes. Six-month outcomes: aortic-related adverse events and the bird-beak phenomenon were observed in 11 (26.8%) and 12 (29.3%) patients, respectively. There was a significant difference in the occurrence of aortic-related adverse events (P=0.036) and bird-beak phenomenon (P=0.002) between groups A and B. In comparison to group B, the aortic-related adverse event rate was significantly higher in group A, with event-free rates of 83.3%, 83.3%, and 72.2% at 1, 3, and 6 months, respectively (P=0.020). Multivariable logistic regression analyses revealed that PLZ LCCA-LSA length [odds ratio (OR) 0.79; 95% CI: 0.64 to 0.97; P=0.026] was significantly associated with the occurrence of the bird-beak configuration, and bird-beak (OR 17.19; 95% CI: 2.24 to 131.81; P=0.006) was a significant risk factor for aortic-related adverse events.

Conclusions

TEVAR with LSA revascularization has good early outcomes. However, it is more susceptible to aortic adverse events when the PLZ LCCA-LSA is less than 10 mm in length. This should be carefully considered, taking into account the risks and benefits.

[Clinicopathological and genetic characteristics of congenital cystic adenomatoid malformation of lung and its associated lung cancer in adults]

Objective: To investigate the clinicopathological features and genetic characteristics of congenital cystic adenomatoid malformation (CCAM) of lung and CCAM associated lung cancer in adults. Methods: A total of 13 cases of CCAM of lung in adults, diagnosed from June 2015 to May 2023, were collected from the Department of Pathology, Shanghai Pulmonary Hospital, Tongji University School of Medicine, China. Their histopathological features were correlated with probable development into lung cancer. Next-generation sequencing was performed on the benign and malignant areas of all cases. Results: The pathological classification of all cases were of CCAM of lung type 1. There were 4 male and 9 female cases, age ranged from 18 to 65 years, with a mean age of 41 years. Six cases were accompanied by lung cancer, all of them were mucinous adenocarcinoma. Next-generation sequencing showed no gene mutation in 2 of the 13 cases; KRAS mutations in exon 2 were detected in 7 cases, in which there were 6 cases complicated with lung mucinous adenocarcinoma and no matter in the malignant or benign regions, the same case exhibited the same mutation sites in KRAS gene. Conclusions: CCAM of the lung is a congenital disease, and in adults, type 1 is most commonly found in the pathological classification, and it is often accompanied by cancer. Gene mutations are frequently detected in CCAM of the lung, KRAS being the most recurrent mutation which may play an important role in the carcinogenesis.

The relationship between dietary inflammatory index and bone mineral density in CKD patients

INTRODUCTION

Chronic systemic inflammation was proposed as a critical factor in the development of osteoporosis. We aim to investigate the effect of the DII on bone mineral density (BMD) in CKD patients.

METHODS

2276 participants from NHANES were enrolled. The DII score was calculated based on a single 24-h dietary recall. Total BMD was measured using Dual-energy x-ray absorptiometry. A multiple-stepwise linear regression model was used to determine associations between BMD and DII in CKD patients.

RESULTS

When DII >0.35, a negative correlation was obtained between DII and BMD (all β = -0.008 and p < 0.05). In subgroup analysis, BMD levels decreased across increasing tertiles of the DII for patients with non-osteoporosis, postmenopause, and low eGFR (p for trend ≤0.01).

CONCLUSION

Higher consumption of pro-inflammatory diet correlates negatively with the BMD levels in CKD patients.

Neural stem cell-derived exosomes regulate cell proliferation, migration, and cell death of brain microvascular endothelial cells via the miR-9/Hes1 axis under hypoxia

BACKGROUND

Our previous study found that mouse embryonic neural stem cell (NSC)-derived exosomes (EXOs) regulated NSC differentiation via the miR-9/Hes1 axis. However, the effects of EXOs on brain microvascular endothelial cell (BMEC) dysfunction via the miR-9/Hes1 axis remain unknown. Therefore, the current study aimed to determine the effects of EXOs on BMEC proliferation, migration, and death via the miR-9/Hes1 axis.

METHODS

Immunofluorescence, quantitative real-time polymerase chain reaction, cell counting kit-8 assay, wound healing assay, calcein-acetoxymethyl/propidium iodide staining, and hematoxylin and eosin staining were used to determine the role and mechanism of EXOs on BMECs.

RESULTS

EXOs promoted BMEC proliferation and migration and reduced cell death under hypoxic conditions. The overexpression of miR-9 promoted BMEC proliferation and migration and reduced cell death under hypoxic conditions. Moreover, miR-9 downregulation inhibited BMEC proliferation and migration and also promoted cell death. Hes1 silencing ameliorated the effect of amtagomiR-9 on BMEC proliferation and migration and cell death. Hyperemic structures were observed in the regions of the hippocampus and cortex in hypoxia-induced mice. Meanwhile, EXO treatment improved cerebrovascular alterations.

CONCLUSION

NSC-derived EXOs can promote BMEC proliferation and migration and reduce cell death via the miR-9/Hes1 axis under hypoxic conditions. Therefore, EXO therapeutic strategies could be considered for hypoxia-induced vascular injury.

Purification and Properties of a Plasmin-like Marine Protease from Clamworm (Perinereis aibuhitensis)

Marine organisms are a rich source of enzymes that exhibit excellent biological activity and a wide range of applications. However, there has been limited research on the proteases found in marine mudflat organisms. Based on this background, the marine fibrinolytic enzyme FELP, which was isolated and purified from clamworm (Perinereis aibuhitensis), has exhibited excellent fibrinolytic activity. We demonstrated the FELP with a purification of 10.61-fold by precipitation with ammonium sulfate, ion-exchange chromatography, and gel-filtration chromatography. SDS-PAGE, fibrin plate method, and LC-MS/MS indicated that the molecular weight of FELP is 28.9 kDa and identified FELP as a fibrinolytic enzyme-like protease. FELP displayed the maximum fibrinolytic activity at pH 9 (407 ± 16 mm2) and 50 °C (724 ± 27 mm2) and had excellent stability at pH 7-11 (50%) or 30-60 °C (60%), respectively. The three-dimensional structure of some amino acid residues of FELP was predicted with the SWISS-MODEL. The fibrinolytic and fibrinogenolytic assays showed that the enzyme possessed direct fibrinolytic activity and indirect fibrinolysis via the activation of plasminogen; it could preferentially degrade Aα-chains of fibrinogen, followed by Bβ- and γ-chains. Overall, the fibrinolytic enzyme was successfully purified from Perinereis aibuhitensis, a marine Annelida (phylum), with favorable stability that has strong fibrinolysis activity in vitro. Therefore, FELP appears to be a potent fibrinolytic enzyme with an application that deserves further investigation.

ψ(2S) Suppression in Pb-Pb Collisions at the LHC

The production of the ψ(2S) charmonium state was measured with ALICE in Pb-Pb collisions at sqrt[s_{NN}]=5.02  TeV, in the dimuon decay channel. A significant signal was observed for the first time at LHC energies down to zero transverse momentum, at forward rapidity (2.5 Collapse

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Affiliation(s)

S Acharya Université Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France
D Adamová Nuclear Physics Institute of the Czech Academy of Sciences, Husinec-Řež, Czech Republic
A Adler Johann-Wolfgang-Goethe Universität Frankfurt Institut für Informatik, Fachbereich Informatik und Mathematik, Frankfurt, Germany
G Aglieri Rinella European Organization for Nuclear Research (CERN), Geneva, Switzerland
M Agnello Dipartimento DISAT del Politecnico and Sezione INFN, Turin, Italy
N Agrawal INFN, Sezione di Bologna, Bologna, Italy
Z Ahammed Variable Energy Cyclotron Centre, Homi Bhabha National Institute, Kolkata, India
S Ahmad Department of Physics, Aligarh Muslim University, Aligarh, India
S U Ahn Korea Institute of Science and Technology Information, Daejeon, Republic of Korea
I Ahuja Faculty of Science, P.J. Šafárik University, Košice, Slovak Republic
A Akindinov Affiliated with an institute covered by a cooperation agreement with CERN
M Al-Turany Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
D Aleksandrov Affiliated with an institute covered by a cooperation agreement with CERN
B Alessandro INFN, Sezione di Torino, Turin, Italy
H M Alfanda Central China Normal University, Wuhan, China
R Alfaro Molina Instituto de Física, Universidad Nacional Autónoma de México, Mexico City, Mexico
B Ali Department of Physics, Aligarh Muslim University, Aligarh, India
A Alici Dipartimento di Fisica e Astronomia dell'Università and Sezione INFN, Bologna, Italy
N Alizadehvandchali University of Houston, Houston, Texas, USA
A Alkin European Organization for Nuclear Research (CERN), Geneva, Switzerland
J Alme Department of Physics and Technology, University of Bergen, Bergen, Norway
G Alocco INFN, Sezione di Cagliari, Cagliari, Italy
T Alt Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
I Altsybeev Affiliated with an institute covered by a cooperation agreement with CERN
M N Anaam Central China Normal University, Wuhan, China
C Andrei Horia Hulubei National Institute of Physics and Nuclear Engineering, Bucharest, Romania
A Andronic Westfälische Wilhelms-Universität Münster, Institut für Kernphysik, Munster, Germany
V Anguelov Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
F Antinori INFN, Sezione di Padova, Padova, Italy
P Antonioli INFN, Sezione di Bologna, Bologna, Italy
N Apadula Lawrence Berkeley National Laboratory, Berkeley, California, USA
L Aphecetche SUBATECH, IMT Atlantique, Nantes Université, CNRS-IN2P3, Nantes, France
H Appelshäuser Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
C Arata Laboratoire de Physique Subatomique et de Cosmologie, Université Grenoble-Alpes, CNRS-IN2P3, Grenoble, France
S Arcelli Dipartimento di Fisica e Astronomia dell'Università and Sezione INFN, Bologna, Italy
M Aresti INFN, Sezione di Cagliari, Cagliari, Italy
R Arnaldi INFN, Sezione di Torino, Turin, Italy
I C Arsene Department of Physics, University of Oslo, Oslo, Norway
M Arslandok Yale University, New Haven, Connecticut, USA
A Augustinus European Organization for Nuclear Research (CERN), Geneva, Switzerland
R Averbeck Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
M D Azmi Department of Physics, Aligarh Muslim University, Aligarh, India
A Badalà INFN, Sezione di Catania, Catania, Italy
J Bae Sungkyunkwan University, Suwon City, Republic of Korea
Y W Baek Gangneung-Wonju National University, Gangneung, Republic of Korea
X Bai University of Science and Technology of China, Hefei, China
R Bailhache Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
Y Bailung Indian Institute of Technology Indore, Indore, India
A Balbino Dipartimento DISAT del Politecnico and Sezione INFN, Turin, Italy
A Baldisseri Université Paris-Saclay Centre d'Etudes de Saclay (CEA), IRFU, Départment de Physique Nucléaire (DPhN), Saclay, France
B Balis AGH University of Science and Technology, Cracow, Poland
D Banerjee Bose Institute, Department of Physics, and Centre for Astroparticle Physics and Space Science (CAPSS), Kolkata, India
Z Banoo Physics Department, University of Jammu, Jammu, India
R Barbera Dipartimento di Fisica e Astronomia dell'Università and Sezione INFN, Catania, Italy
F Barile Dipartimento Interateneo di Fisica 'M. Merlin' and Sezione INFN, Bari, Italy
L Barioglio Physik Department, Technische Universität München, Munich, Germany
M Barlou National and Kapodistrian University of Athens, School of Science, Department of Physics, Athens, Greece
G G Barnaföldi Wigner Research Centre for Physics, Budapest, Hungary
L S Barnby Nuclear Physics Group, STFC Daresbury Laboratory, Daresbury, United Kingdom
V Barret Université Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France
L Barreto Universidade de São Paulo (USP), São Paulo, Brazil
C Bartels University of Liverpool, Liverpool, United Kingdom
K Barth European Organization for Nuclear Research (CERN), Geneva, Switzerland
E Bartsch Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
F Baruffaldi Dipartimento di Fisica e Astronomia dell'Università and Sezione INFN, Padova, Italy
N Bastid Université Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France
S Basu Lund University Department of Physics, Division of Particle Physics, Lund, Sweden
G Batigne SUBATECH, IMT Atlantique, Nantes Université, CNRS-IN2P3, Nantes, France
D Battistini Physik Department, Technische Universität München, Munich, Germany
B Batyunya Affiliated with an international laboratory covered by a cooperation agreement with CERN
D Bauri Indian Institute of Technology Bombay (IIT), Mumbai, India
J L Bazo Alba Sección Física, Departamento de Ciencias, Pontificia Universidad Católica del Perú, Lima, Peru
I G Bearden Niels Bohr Institute, University of Copenhagen, Copenhagen, Denmark
C Beattie Yale University, New Haven, Connecticut, USA
P Becht Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
D Behera Indian Institute of Technology Indore, Indore, India
I Belikov Université de Strasbourg, CNRS, IPHC UMR 7178, F-67000 Strasbourg, France, Strasbourg, France
A D C Bell Hechavarria Westfälische Wilhelms-Universität Münster, Institut für Kernphysik, Munster, Germany
F Bellini Dipartimento di Fisica e Astronomia dell'Università and Sezione INFN, Bologna, Italy
R Bellwied University of Houston, Houston, Texas, USA
S Belokurova Affiliated with an institute covered by a cooperation agreement with CERN
V Belyaev Affiliated with an institute covered by a cooperation agreement with CERN
G Bencedi Wigner Research Centre for Physics, Budapest, Hungary
S Beole Dipartimento di Fisica dell'Università and Sezione INFN, Turin, Italy
A Bercuci Horia Hulubei National Institute of Physics and Nuclear Engineering, Bucharest, Romania
Y Berdnikov Affiliated with an institute covered by a cooperation agreement with CERN
A Berdnikova Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
L Bergmann Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
M G Besoiu Institute of Space Science (ISS), Bucharest, Romania
L Betev European Organization for Nuclear Research (CERN), Geneva, Switzerland
P P Bhaduri Variable Energy Cyclotron Centre, Homi Bhabha National Institute, Kolkata, India
A Bhasin Physics Department, University of Jammu, Jammu, India
M A Bhat Bose Institute, Department of Physics, and Centre for Astroparticle Physics and Space Science (CAPSS), Kolkata, India
B Bhattacharjee Gauhati University, Department of Physics, Guwahati, India
L Bianchi Dipartimento di Fisica dell'Università and Sezione INFN, Turin, Italy
N Bianchi INFN, Laboratori Nazionali di Frascati, Frascati, Italy
J Bielčík Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic
J Bielčíková Nuclear Physics Institute of the Czech Academy of Sciences, Husinec-Řež, Czech Republic
J Biernat The Henryk Niewodniczanski Institute of Nuclear Physics, Polish Academy of Sciences, Cracow, Poland
A P Bigot Université de Strasbourg, CNRS, IPHC UMR 7178, F-67000 Strasbourg, France, Strasbourg, France
A Bilandzic Physik Department, Technische Universität München, Munich, Germany
G Biro Wigner Research Centre for Physics, Budapest, Hungary
S Biswas Bose Institute, Department of Physics, and Centre for Astroparticle Physics and Space Science (CAPSS), Kolkata, India
N Bize SUBATECH, IMT Atlantique, Nantes Université, CNRS-IN2P3, Nantes, France
J T Blair The University of Texas at Austin, Austin, Texas, USA
D Blau Affiliated with an institute covered by a cooperation agreement with CERN
M B Blidaru Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
N Bluhme Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
C Blume Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
G Boca Dipartimento di Fisica, Università di Pavia, Pavia, Italy INFN, Sezione di Pavia, Pavia, Italy
F Bock Oak Ridge National Laboratory, Oak Ridge, Tennessee, USA
T Bodova Department of Physics and Technology, University of Bergen, Bergen, Norway
A Bogdanov Affiliated with an institute covered by a cooperation agreement with CERN
S Boi Dipartimento di Fisica dell'Università and Sezione INFN, Cagliari, Italy
J Bok Inha University, Incheon, Republic of Korea
L Boldizsár Wigner Research Centre for Physics, Budapest, Hungary
A Bolozdynya Affiliated with an institute covered by a cooperation agreement with CERN
M Bombara Faculty of Science, P.J. Šafárik University, Košice, Slovak Republic
P M Bond European Organization for Nuclear Research (CERN), Geneva, Switzerland
G Bonomi INFN, Sezione di Pavia, Pavia, Italy Università di Brescia, Brescia, Italy
H Borel Université Paris-Saclay Centre d'Etudes de Saclay (CEA), IRFU, Départment de Physique Nucléaire (DPhN), Saclay, France
A Borissov Affiliated with an institute covered by a cooperation agreement with CERN
A G Borquez Carcamo Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
H Bossi Yale University, New Haven, Connecticut, USA
E Botta Dipartimento di Fisica dell'Università and Sezione INFN, Turin, Italy
Y E M Bouziani Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
L Bratrud Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
P Braun-Munzinger Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
M Bregant Universidade de São Paulo (USP), São Paulo, Brazil
M Broz Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic
G E Bruno Dipartimento Interateneo di Fisica 'M. Merlin' and Sezione INFN, Bari, Italy Politecnico di Bari and Sezione INFN, Bari, Italy
D Budnikov Affiliated with an institute covered by a cooperation agreement with CERN
H Buesching Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
S Bufalino Dipartimento DISAT del Politecnico and Sezione INFN, Turin, Italy
O Bugnon SUBATECH, IMT Atlantique, Nantes Université, CNRS-IN2P3, Nantes, France
P Buhler Stefan Meyer Institut für Subatomare Physik (SMI), Vienna, Austria
Z Buthelezi iThemba LABS, National Research Foundation, Somerset West, South Africa University of the Witwatersrand, Johannesburg, South Africa
S A Bysiak The Henryk Niewodniczanski Institute of Nuclear Physics, Polish Academy of Sciences, Cracow, Poland
M Cai Central China Normal University, Wuhan, China
H Caines Yale University, New Haven, Connecticut, USA
A Caliva Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
E Calvo Villar Sección Física, Departamento de Ciencias, Pontificia Universidad Católica del Perú, Lima, Peru
J M M Camacho Universidad Autónoma de Sinaloa, Culiacan, Mexico
P Camerini Dipartimento di Fisica dell'Università and Sezione INFN, Trieste, Italy
F D M Canedo Universidade de São Paulo (USP), São Paulo, Brazil
M Carabas University Politehnica of Bucharest, Bucharest, Romania
A A Carballo European Organization for Nuclear Research (CERN), Geneva, Switzerland
F Carnesecchi European Organization for Nuclear Research (CERN), Geneva, Switzerland
R Caron Université de Lyon, CNRS/IN2P3, Institut de Physique des 2 Infinis de Lyon, Lyon, France
J Castillo Castellanos Université Paris-Saclay Centre d'Etudes de Saclay (CEA), IRFU, Départment de Physique Nucléaire (DPhN), Saclay, France
F Catalano Dipartimento di Fisica dell'Università and Sezione INFN, Turin, Italy Dipartimento DISAT del Politecnico and Sezione INFN, Turin, Italy
C Ceballos Sanchez Affiliated with an international laboratory covered by a cooperation agreement with CERN
I Chakaberia Lawrence Berkeley National Laboratory, Berkeley, California, USA
P Chakraborty Indian Institute of Technology Bombay (IIT), Mumbai, India
S Chandra Variable Energy Cyclotron Centre, Homi Bhabha National Institute, Kolkata, India
S Chapeland European Organization for Nuclear Research (CERN), Geneva, Switzerland
M Chartier University of Liverpool, Liverpool, United Kingdom
S Chattopadhyay Variable Energy Cyclotron Centre, Homi Bhabha National Institute, Kolkata, India
S Chattopadhyay Saha Institute of Nuclear Physics, Homi Bhabha National Institute, Kolkata, India
T G Chavez High Energy Physics Group, Universidad Autónoma de Puebla, Puebla, Mexico
T Cheng Central China Normal University, Wuhan, China Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
C Cheshkov Université de Lyon, CNRS/IN2P3, Institut de Physique des 2 Infinis de Lyon, Lyon, France
B Cheynis Université de Lyon, CNRS/IN2P3, Institut de Physique des 2 Infinis de Lyon, Lyon, France
V Chibante Barroso European Organization for Nuclear Research (CERN), Geneva, Switzerland
D D Chinellato Universidade Estadual de Campinas (UNICAMP), Campinas, Brazil
E S Chizzali Physik Department, Technische Universität München, Munich, Germany
J Cho Inha University, Incheon, Republic of Korea
S Cho Inha University, Incheon, Republic of Korea
P Chochula European Organization for Nuclear Research (CERN), Geneva, Switzerland
P Christakoglou Nikhef, National institute for subatomic physics, Amsterdam, Netherlands
C H Christensen Niels Bohr Institute, University of Copenhagen, Copenhagen, Denmark
P Christiansen Lund University Department of Physics, Division of Particle Physics, Lund, Sweden
T Chujo University of Tsukuba, Tsukuba, Japan
M Ciacco Dipartimento DISAT del Politecnico and Sezione INFN, Turin, Italy
C Cicalo INFN, Sezione di Cagliari, Cagliari, Italy
F Cindolo INFN, Sezione di Bologna, Bologna, Italy
M R Ciupek Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
G Clai INFN, Sezione di Bologna, Bologna, Italy
F Colamaria INFN, Sezione di Bari, Bari, Italy
J S Colburn School of Physics and Astronomy, University of Birmingham, Birmingham, United Kingdom
D Colella Dipartimento Interateneo di Fisica 'M. Merlin' and Sezione INFN, Bari, Italy Politecnico di Bari and Sezione INFN, Bari, Italy
M Colocci European Organization for Nuclear Research (CERN), Geneva, Switzerland
M Concas INFN, Sezione di Torino, Turin, Italy
G Conesa Balbastre Laboratoire de Physique Subatomique et de Cosmologie, Université Grenoble-Alpes, CNRS-IN2P3, Grenoble, France
Z Conesa Del Valle Laboratoire de Physique des 2 Infinis, Irène Joliot-Curie, Orsay, France
G Contin Dipartimento di Fisica dell'Università and Sezione INFN, Trieste, Italy
J G Contreras Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic
M L Coquet Université Paris-Saclay Centre d'Etudes de Saclay (CEA), IRFU, Départment de Physique Nucléaire (DPhN), Saclay, France
T M Cormier Oak Ridge National Laboratory, Oak Ridge, Tennessee, USA
P Cortese INFN, Sezione di Torino, Turin, Italy Università del Piemonte Orientale, Vercelli, Italy
M R Cosentino Universidade Federal do ABC, Santo Andre, Brazil
F Costa European Organization for Nuclear Research (CERN), Geneva, Switzerland
S Costanza Dipartimento di Fisica, Università di Pavia, Pavia, Italy INFN, Sezione di Pavia, Pavia, Italy
J Crkovská Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
P Crochet Université Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France
R Cruz-Torres Lawrence Berkeley National Laboratory, Berkeley, California, USA
E Cuautle Instituto de Ciencias Nucleares, Universidad Nacional Autónoma de México, Mexico City, Mexico
P Cui Central China Normal University, Wuhan, China
A Dainese INFN, Sezione di Padova, Padova, Italy
M C Danisch Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
A Danu Institute of Space Science (ISS), Bucharest, Romania
P Das National Institute of Science Education and Research, Homi Bhabha National Institute, Jatni, India
P Das Bose Institute, Department of Physics, and Centre for Astroparticle Physics and Space Science (CAPSS), Kolkata, India
S Das Bose Institute, Department of Physics, and Centre for Astroparticle Physics and Space Science (CAPSS), Kolkata, India
A R Dash Westfälische Wilhelms-Universität Münster, Institut für Kernphysik, Munster, Germany
S Dash Indian Institute of Technology Bombay (IIT), Mumbai, India
A De Caro Dipartimento di Fisica 'E.R. Caianiello' dell' Università and Gruppo Collegato INFN, Salerno, Italy
G de Cataldo INFN, Sezione di Bari, Bari, Italy
J de Cuveland Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
A De Falco Dipartimento di Fisica dell'Università and Sezione INFN, Cagliari, Italy
D De Gruttola Dipartimento di Fisica 'E.R. Caianiello' dell' Università and Gruppo Collegato INFN, Salerno, Italy
N De Marco INFN, Sezione di Torino, Turin, Italy
C De Martin Dipartimento di Fisica dell'Università and Sezione INFN, Trieste, Italy
S De Pasquale Dipartimento di Fisica 'E.R. Caianiello' dell' Università and Gruppo Collegato INFN, Salerno, Italy
S Deb Indian Institute of Technology Indore, Indore, India
R J Debski AGH University of Science and Technology, Cracow, Poland
K R Deja Warsaw University of Technology, Warsaw, Poland
R Del Grande Physik Department, Technische Universität München, Munich, Germany
L Dello Stritto Dipartimento di Fisica 'E.R. Caianiello' dell' Università and Gruppo Collegato INFN, Salerno, Italy
W Deng Central China Normal University, Wuhan, China
P Dhankher Department of Physics, University of California, Berkeley, California, USA
D Di Bari Dipartimento Interateneo di Fisica 'M. Merlin' and Sezione INFN, Bari, Italy
A Di Mauro European Organization for Nuclear Research (CERN), Geneva, Switzerland
R A Diaz Centro de Aplicaciones Tecnológicas y Desarrollo Nuclear (CEADEN), Havana, Cuba Affiliated with an international laboratory covered by a cooperation agreement with CERN
T Dietel University of Cape Town, Cape Town, South Africa
Y Ding Central China Normal University, Wuhan, China Université de Lyon, CNRS/IN2P3, Institut de Physique des 2 Infinis de Lyon, Lyon, France
R Divià European Organization for Nuclear Research (CERN), Geneva, Switzerland
D U Dixit Department of Physics, University of California, Berkeley, California, USA
Ø Djuvsland Department of Physics and Technology, University of Bergen, Bergen, Norway
U Dmitrieva Affiliated with an institute covered by a cooperation agreement with CERN
A Dobrin Institute of Space Science (ISS), Bucharest, Romania
B Dönigus Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
J M Dubinski Warsaw University of Technology, Warsaw, Poland
A Dubla Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
S Dudi Physics Department, Panjab University, Chandigarh, India
P Dupieux Université Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France
M Durkac Technical University of Košice, Košice, Slovak Republic
N Dzalaiova Comenius University Bratislava, Faculty of Mathematics, Physics and Informatics, Bratislava, Slovak Republic
T M Eder Westfälische Wilhelms-Universität Münster, Institut für Kernphysik, Munster, Germany
R J Ehlers Oak Ridge National Laboratory, Oak Ridge, Tennessee, USA
V N Eikeland Department of Physics and Technology, University of Bergen, Bergen, Norway
F Eisenhut Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
D Elia INFN, Sezione di Bari, Bari, Italy
B Erazmus SUBATECH, IMT Atlantique, Nantes Université, CNRS-IN2P3, Nantes, France
F Ercolessi Dipartimento di Fisica e Astronomia dell'Università and Sezione INFN, Bologna, Italy
F Erhardt Physics department, Faculty of science, University of Zagreb, Zagreb, Croatia
M R Ersdal Department of Physics and Technology, University of Bergen, Bergen, Norway
B Espagnon Laboratoire de Physique des 2 Infinis, Irène Joliot-Curie, Orsay, France
G Eulisse European Organization for Nuclear Research (CERN), Geneva, Switzerland
D Evans School of Physics and Astronomy, University of Birmingham, Birmingham, United Kingdom
S Evdokimov Affiliated with an institute covered by a cooperation agreement with CERN
L Fabbietti Physik Department, Technische Universität München, Munich, Germany
M Faggin Dipartimento di Fisica e Astronomia dell'Università and Sezione INFN, Padova, Italy
J Faivre Laboratoire de Physique Subatomique et de Cosmologie, Université Grenoble-Alpes, CNRS-IN2P3, Grenoble, France
F Fan Central China Normal University, Wuhan, China
W Fan Lawrence Berkeley National Laboratory, Berkeley, California, USA
A Fantoni INFN, Laboratori Nazionali di Frascati, Frascati, Italy
M Fasel Oak Ridge National Laboratory, Oak Ridge, Tennessee, USA
P Fecchio Dipartimento DISAT del Politecnico and Sezione INFN, Turin, Italy
A Feliciello INFN, Sezione di Torino, Turin, Italy
G Feofilov Affiliated with an institute covered by a cooperation agreement with CERN
A Fernández Téllez High Energy Physics Group, Universidad Autónoma de Puebla, Puebla, Mexico
L Ferrandi Universidade de São Paulo (USP), São Paulo, Brazil
M B Ferrer European Organization for Nuclear Research (CERN), Geneva, Switzerland
A Ferrero Université Paris-Saclay Centre d'Etudes de Saclay (CEA), IRFU, Départment de Physique Nucléaire (DPhN), Saclay, France
C Ferrero INFN, Sezione di Torino, Turin, Italy
A Ferretti Dipartimento di Fisica dell'Università and Sezione INFN, Turin, Italy
V J G Feuillard Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
V Filova Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic
D Finogeev Affiliated with an institute covered by a cooperation agreement with CERN
F M Fionda INFN, Sezione di Cagliari, Cagliari, Italy
F Flor University of Houston, Houston, Texas, USA
A N Flores The University of Texas at Austin, Austin, Texas, USA
S Foertsch iThemba LABS, National Research Foundation, Somerset West, South Africa
I Fokin Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
S Fokin Affiliated with an institute covered by a cooperation agreement with CERN
E Fragiacomo INFN, Sezione di Trieste, Trieste, Italy
E Frajna Wigner Research Centre for Physics, Budapest, Hungary
U Fuchs European Organization for Nuclear Research (CERN), Geneva, Switzerland
N Funicello Dipartimento di Fisica 'E.R. Caianiello' dell' Università and Gruppo Collegato INFN, Salerno, Italy
C Furget Laboratoire de Physique Subatomique et de Cosmologie, Université Grenoble-Alpes, CNRS-IN2P3, Grenoble, France
A Furs Affiliated with an institute covered by a cooperation agreement with CERN
T Fusayasu Saga University, Saga, Japan
J J Gaardhøje Niels Bohr Institute, University of Copenhagen, Copenhagen, Denmark
M Gagliardi Dipartimento di Fisica dell'Università and Sezione INFN, Turin, Italy
A M Gago Sección Física, Departamento de Ciencias, Pontificia Universidad Católica del Perú, Lima, Peru
C D Galvan Universidad Autónoma de Sinaloa, Culiacan, Mexico
D R Gangadharan University of Houston, Houston, Texas, USA
P Ganoti National and Kapodistrian University of Athens, School of Science, Department of Physics, Athens, Greece
C Garabatos Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
J R A Garcia High Energy Physics Group, Universidad Autónoma de Puebla, Puebla, Mexico
E Garcia-Solis Chicago State University, Chicago, Illinois, USA
K Garg SUBATECH, IMT Atlantique, Nantes Université, CNRS-IN2P3, Nantes, France
C Gargiulo European Organization for Nuclear Research (CERN), Geneva, Switzerland
A Garibli National Nuclear Research Center, Baku, Azerbaijan
K Garner Westfälische Wilhelms-Universität Münster, Institut für Kernphysik, Munster, Germany
P Gasik Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
A Gautam University of Kansas, Lawrence, Kansas, USA
M B Gay Ducati Instituto de Física, Universidade Federal do Rio Grande do Sul (UFRGS), Porto Alegre, Brazil
M Germain SUBATECH, IMT Atlantique, Nantes Université, CNRS-IN2P3, Nantes, France
C Ghosh Variable Energy Cyclotron Centre, Homi Bhabha National Institute, Kolkata, India
M Giacalone Dipartimento di Fisica e Astronomia dell'Università and Sezione INFN, Bologna, Italy
P Giubellino INFN, Sezione di Torino, Turin, Italy Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
P Giubilato Dipartimento di Fisica e Astronomia dell'Università and Sezione INFN, Padova, Italy
A M C Glaenzer Université Paris-Saclay Centre d'Etudes de Saclay (CEA), IRFU, Départment de Physique Nucléaire (DPhN), Saclay, France
P Glässel Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
E Glimos University of Tennessee, Knoxville, Tennessee, USA
D J Q Goh Nagasaki Institute of Applied Science, Nagasaki, Japan
V Gonzalez Wayne State University, Detroit, Michigan, USA
L H González-Trueba Instituto de Física, Universidad Nacional Autónoma de México, Mexico City, Mexico
M Gorgon AGH University of Science and Technology, Cracow, Poland
S Gotovac Faculty of Electrical Engineering, Mechanical Engineering and Naval Architecture, University of Split, Split, Croatia
V Grabski Instituto de Física, Universidad Nacional Autónoma de México, Mexico City, Mexico
L K Graczykowski Warsaw University of Technology, Warsaw, Poland
E Grecka Nuclear Physics Institute of the Czech Academy of Sciences, Husinec-Řež, Czech Republic
A Grelli Institute for Gravitational and Subatomic Physics (GRASP), Utrecht University/Nikhef, Utrecht, Netherlands
C Grigoras European Organization for Nuclear Research (CERN), Geneva, Switzerland
V Grigoriev Affiliated with an institute covered by a cooperation agreement with CERN
S Grigoryan A.I. Alikhanyan National Science Laboratory (Yerevan Physics Institute) Foundation, Yerevan, Armenia Affiliated with an international laboratory covered by a cooperation agreement with CERN
F Grosa European Organization for Nuclear Research (CERN), Geneva, Switzerland
J F Grosse-Oetringhaus European Organization for Nuclear Research (CERN), Geneva, Switzerland
R Grosso Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
D Grund Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic
G G Guardiano Universidade Estadual de Campinas (UNICAMP), Campinas, Brazil
R Guernane Laboratoire de Physique Subatomique et de Cosmologie, Université Grenoble-Alpes, CNRS-IN2P3, Grenoble, France
M Guilbaud SUBATECH, IMT Atlantique, Nantes Université, CNRS-IN2P3, Nantes, France
K Gulbrandsen Niels Bohr Institute, University of Copenhagen, Copenhagen, Denmark
T Gundem Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
T Gunji University of Tokyo, Tokyo, Japan
W Guo Central China Normal University, Wuhan, China
A Gupta Physics Department, University of Jammu, Jammu, India
R Gupta Physics Department, University of Jammu, Jammu, India
S P Guzman High Energy Physics Group, Universidad Autónoma de Puebla, Puebla, Mexico
L Gyulai Wigner Research Centre for Physics, Budapest, Hungary
M K Habib Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
C Hadjidakis Laboratoire de Physique des 2 Infinis, Irène Joliot-Curie, Orsay, France
F U Haider Physics Department, University of Jammu, Jammu, India
H Hamagaki Nagasaki Institute of Applied Science, Nagasaki, Japan
A Hamdi Lawrence Berkeley National Laboratory, Berkeley, California, USA
M Hamid Central China Normal University, Wuhan, China
Y Han Yonsei University, Seoul, Republic of Korea
R Hannigan The University of Texas at Austin, Austin, Texas, USA
M R Haque Warsaw University of Technology, Warsaw, Poland
J W Harris Yale University, New Haven, Connecticut, USA
A Harton Chicago State University, Chicago, Illinois, USA
H Hassan Oak Ridge National Laboratory, Oak Ridge, Tennessee, USA
D Hatzifotiadou INFN, Sezione di Bologna, Bologna, Italy
P Hauer Helmholtz-Institut für Strahlen- und Kernphysik, Rheinische Friedrich-Wilhelms-Universität Bonn, Bonn, Germany
L B Havener Yale University, New Haven, Connecticut, USA
S T Heckel Physik Department, Technische Universität München, Munich, Germany
E Hellbär Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
H Helstrup Faculty of Engineering and Science, Western Norway University of Applied Sciences, Bergen, Norway
M Hemmer Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
T Herman Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic
G Herrera Corral Centro de Investigación y de Estudios Avanzados (CINVESTAV), Mexico City and Merida, Mexico
F Herrmann Westfälische Wilhelms-Universität Münster, Institut für Kernphysik, Munster, Germany
S Herrmann Université de Lyon, CNRS/IN2P3, Institut de Physique des 2 Infinis de Lyon, Lyon, France
K F Hetland Faculty of Engineering and Science, Western Norway University of Applied Sciences, Bergen, Norway
B Heybeck Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
H Hillemanns European Organization for Nuclear Research (CERN), Geneva, Switzerland
C Hills University of Liverpool, Liverpool, United Kingdom
B Hippolyte Université de Strasbourg, CNRS, IPHC UMR 7178, F-67000 Strasbourg, France, Strasbourg, France
B Hofman Institute for Gravitational and Subatomic Physics (GRASP), Utrecht University/Nikhef, Utrecht, Netherlands
B Hohlweger Nikhef, National institute for subatomic physics, Amsterdam, Netherlands
G H Hong Yonsei University, Seoul, Republic of Korea
M Horst Physik Department, Technische Universität München, Munich, Germany
A Horzyk AGH University of Science and Technology, Cracow, Poland
R Hosokawa Creighton University, Omaha, Nebraska, USA
Y Hou Central China Normal University, Wuhan, China
P Hristov European Organization for Nuclear Research (CERN), Geneva, Switzerland
C Hughes University of Tennessee, Knoxville, Tennessee, USA
P Huhn Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
L M Huhta University of Jyväskylä, Jyväskylä, Finland
C V Hulse Laboratoire de Physique des 2 Infinis, Irène Joliot-Curie, Orsay, France
T J Humanic Ohio State University, Columbus, Ohio, USA
H Hushnud Department of Physics, Aligarh Muslim University, Aligarh, India Saha Institute of Nuclear Physics, Homi Bhabha National Institute, Kolkata, India
A Hutson University of Houston, Houston, Texas, USA
D Hutter Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
J P Iddon University of Liverpool, Liverpool, United Kingdom
R Ilkaev Affiliated with an institute covered by a cooperation agreement with CERN
H Ilyas COMSATS University Islamabad, Islamabad, Pakistan
M Inaba University of Tsukuba, Tsukuba, Japan
G M Innocenti European Organization for Nuclear Research (CERN), Geneva, Switzerland
M Ippolitov Affiliated with an institute covered by a cooperation agreement with CERN
A Isakov Nuclear Physics Institute of the Czech Academy of Sciences, Husinec-Řež, Czech Republic
T Isidori University of Kansas, Lawrence, Kansas, USA
M S Islam Saha Institute of Nuclear Physics, Homi Bhabha National Institute, Kolkata, India
M Ivanov Comenius University Bratislava, Faculty of Mathematics, Physics and Informatics, Bratislava, Slovak Republic
M Ivanov Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
V Ivanov Affiliated with an institute covered by a cooperation agreement with CERN
M Jablonski AGH University of Science and Technology, Cracow, Poland
B Jacak Lawrence Berkeley National Laboratory, Berkeley, California, USA
N Jacazio European Organization for Nuclear Research (CERN), Geneva, Switzerland
P M Jacobs Lawrence Berkeley National Laboratory, Berkeley, California, USA
S Jadlovska Technical University of Košice, Košice, Slovak Republic
J Jadlovsky Technical University of Košice, Košice, Slovak Republic
S Jaelani National Research and Innovation Agency - BRIN, Jakarta, Indonesia
L Jaffe Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
C Jahnke Universidade Estadual de Campinas (UNICAMP), Campinas, Brazil
M J Jakubowska Warsaw University of Technology, Warsaw, Poland
M A Janik Warsaw University of Technology, Warsaw, Poland
T Janson Johann-Wolfgang-Goethe Universität Frankfurt Institut für Informatik, Fachbereich Informatik und Mathematik, Frankfurt, Germany
M Jercic Physics department, Faculty of science, University of Zagreb, Zagreb, Croatia
S Jia China Institute of Atomic Energy, Beijing, China
A A P Jimenez Instituto de Ciencias Nucleares, Universidad Nacional Autónoma de México, Mexico City, Mexico
F Jonas Oak Ridge National Laboratory, Oak Ridge, Tennessee, USA
J M Jowett European Organization for Nuclear Research (CERN), Geneva, Switzerland Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
J Jung Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
M Jung Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
A Junique European Organization for Nuclear Research (CERN), Geneva, Switzerland
A Jusko School of Physics and Astronomy, University of Birmingham, Birmingham, United Kingdom
M J Kabus European Organization for Nuclear Research (CERN), Geneva, Switzerland Warsaw University of Technology, Warsaw, Poland
J Kaewjai Suranaree University of Technology, Nakhon Ratchasima, Thailand
P Kalinak Institute of Experimental Physics, Slovak Academy of Sciences, Košice, Slovak Republic
A S Kalteyer Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
A Kalweit European Organization for Nuclear Research (CERN), Geneva, Switzerland
V Kaplin Affiliated with an institute covered by a cooperation agreement with CERN
A Karasu Uysal KTO Karatay University, Konya, Turkey
D Karatovic Physics department, Faculty of science, University of Zagreb, Zagreb, Croatia
O Karavichev Affiliated with an institute covered by a cooperation agreement with CERN
T Karavicheva Affiliated with an institute covered by a cooperation agreement with CERN
P Karczmarczyk Warsaw University of Technology, Warsaw, Poland
E Karpechev Affiliated with an institute covered by a cooperation agreement with CERN
U Kebschull Johann-Wolfgang-Goethe Universität Frankfurt Institut für Informatik, Fachbereich Informatik und Mathematik, Frankfurt, Germany
R Keidel Zentrum für Technologie und Transfer (ZTT), Worms, Germany
D L D Keijdener Institute for Gravitational and Subatomic Physics (GRASP), Utrecht University/Nikhef, Utrecht, Netherlands
M Keil European Organization for Nuclear Research (CERN), Geneva, Switzerland
B Ketzer Helmholtz-Institut für Strahlen- und Kernphysik, Rheinische Friedrich-Wilhelms-Universität Bonn, Bonn, Germany
A M Khan Central China Normal University, Wuhan, China
S Khan Department of Physics, Aligarh Muslim University, Aligarh, India
A Khanzadeev Affiliated with an institute covered by a cooperation agreement with CERN
Y Kharlov Affiliated with an institute covered by a cooperation agreement with CERN
A Khatun Department of Physics, Aligarh Muslim University, Aligarh, India University of Kansas, Lawrence, Kansas, USA
A Khuntia The Henryk Niewodniczanski Institute of Nuclear Physics, Polish Academy of Sciences, Cracow, Poland
M B Kidson University of Cape Town, Cape Town, South Africa
B Kileng Faculty of Engineering and Science, Western Norway University of Applied Sciences, Bergen, Norway
B Kim Department of Physics, Pusan National University, Pusan, Republic of Korea
C Kim Department of Physics, Pusan National University, Pusan, Republic of Korea
D J Kim University of Jyväskylä, Jyväskylä, Finland
E J Kim Jeonbuk National University, Jeonju, Republic of Korea
J Kim Yonsei University, Seoul, Republic of Korea
J S Kim Gangneung-Wonju National University, Gangneung, Republic of Korea
J Kim Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
J Kim Jeonbuk National University, Jeonju, Republic of Korea
M Kim Department of Physics, University of California, Berkeley, California, USA Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
S Kim Department of Physics, Sejong University, Seoul, Republic of Korea
T Kim Yonsei University, Seoul, Republic of Korea
K Kimura Physics Program and International Institute for Sustainability with Knotted Chiral Meta Matter (SKCM2), Hiroshima University, Hiroshima, Japan
S Kirsch Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
I Kisel Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
S Kiselev Affiliated with an institute covered by a cooperation agreement with CERN
A Kisiel Warsaw University of Technology, Warsaw, Poland
J P Kitowski AGH University of Science and Technology, Cracow, Poland
J L Klay California Polytechnic State University, San Luis Obispo, California, USA
J Klein European Organization for Nuclear Research (CERN), Geneva, Switzerland
S Klein Lawrence Berkeley National Laboratory, Berkeley, California, USA
C Klein-Bösing Westfälische Wilhelms-Universität Münster, Institut für Kernphysik, Munster, Germany
M Kleiner Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
T Klemenz Physik Department, Technische Universität München, Munich, Germany
A Kluge European Organization for Nuclear Research (CERN), Geneva, Switzerland
A G Knospe University of Houston, Houston, Texas, USA
C Kobdaj Suranaree University of Technology, Nakhon Ratchasima, Thailand
T Kollegger Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
A Kondratyev Affiliated with an international laboratory covered by a cooperation agreement with CERN
E Kondratyuk Affiliated with an institute covered by a cooperation agreement with CERN
J Konig Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
S A Konigstorfer Physik Department, Technische Universität München, Munich, Germany
P J Konopka European Organization for Nuclear Research (CERN), Geneva, Switzerland
G Kornakov Warsaw University of Technology, Warsaw, Poland
S D Koryciak AGH University of Science and Technology, Cracow, Poland
A Kotliarov Nuclear Physics Institute of the Czech Academy of Sciences, Husinec-Řež, Czech Republic
V Kovalenko Affiliated with an institute covered by a cooperation agreement with CERN
M Kowalski The Henryk Niewodniczanski Institute of Nuclear Physics, Polish Academy of Sciences, Cracow, Poland
V Kozhuharov Faculty of Physics, Sofia University, Sofia, Bulgaria
I Králik Institute of Experimental Physics, Slovak Academy of Sciences, Košice, Slovak Republic
A Kravčáková Faculty of Science, P.J. Šafárik University, Košice, Slovak Republic
L Kreis Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
M Krivda Institute of Experimental Physics, Slovak Academy of Sciences, Košice, Slovak Republic School of Physics and Astronomy, University of Birmingham, Birmingham, United Kingdom
F Krizek Nuclear Physics Institute of the Czech Academy of Sciences, Husinec-Řež, Czech Republic
K Krizkova Gajdosova Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic
M Kroesen Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
M Krüger Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
D M Krupova Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic
E Kryshen Affiliated with an institute covered by a cooperation agreement with CERN
V Kučera European Organization for Nuclear Research (CERN), Geneva, Switzerland
C Kuhn Université de Strasbourg, CNRS, IPHC UMR 7178, F-67000 Strasbourg, France, Strasbourg, France
P G Kuijer Nikhef, National institute for subatomic physics, Amsterdam, Netherlands
T Kumaoka University of Tsukuba, Tsukuba, Japan
D Kumar Variable Energy Cyclotron Centre, Homi Bhabha National Institute, Kolkata, India
L Kumar Physics Department, Panjab University, Chandigarh, India
N Kumar Physics Department, Panjab University, Chandigarh, India
S Kumar Dipartimento Interateneo di Fisica 'M. Merlin' and Sezione INFN, Bari, Italy
S Kundu European Organization for Nuclear Research (CERN), Geneva, Switzerland
P Kurashvili National Centre for Nuclear Research, Warsaw, Poland
A Kurepin Affiliated with an institute covered by a cooperation agreement with CERN
A B Kurepin Affiliated with an institute covered by a cooperation agreement with CERN
A Kuryakin Affiliated with an institute covered by a cooperation agreement with CERN
S Kushpil Nuclear Physics Institute of the Czech Academy of Sciences, Husinec-Řež, Czech Republic
J Kvapil School of Physics and Astronomy, University of Birmingham, Birmingham, United Kingdom
M J Kweon Inha University, Incheon, Republic of Korea
J Y Kwon Inha University, Incheon, Republic of Korea
Y Kwon Yonsei University, Seoul, Republic of Korea
S L La Pointe Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
P La Rocca Dipartimento di Fisica e Astronomia dell'Università and Sezione INFN, Catania, Italy
Y S Lai Lawrence Berkeley National Laboratory, Berkeley, California, USA
A Lakrathok Suranaree University of Technology, Nakhon Ratchasima, Thailand
M Lamanna European Organization for Nuclear Research (CERN), Geneva, Switzerland
R Langoy University of South-Eastern Norway, Kongsberg, Norway
P Larionov European Organization for Nuclear Research (CERN), Geneva, Switzerland
E Laudi European Organization for Nuclear Research (CERN), Geneva, Switzerland
L Lautner European Organization for Nuclear Research (CERN), Geneva, Switzerland Physik Department, Technische Universität München, Munich, Germany
R Lavicka Stefan Meyer Institut für Subatomare Physik (SMI), Vienna, Austria
T Lazareva Affiliated with an institute covered by a cooperation agreement with CERN
R Lea INFN, Sezione di Pavia, Pavia, Italy Università di Brescia, Brescia, Italy
H Lee Sungkyunkwan University, Suwon City, Republic of Korea
G Legras Westfälische Wilhelms-Universität Münster, Institut für Kernphysik, Munster, Germany
J Lehrbach Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
R C Lemmon Nuclear Physics Group, STFC Daresbury Laboratory, Daresbury, United Kingdom
I León Monzón Universidad Autónoma de Sinaloa, Culiacan, Mexico
M M Lesch Physik Department, Technische Universität München, Munich, Germany
E D Lesser Department of Physics, University of California, Berkeley, California, USA
M Lettrich Physik Department, Technische Universität München, Munich, Germany
P Lévai Wigner Research Centre for Physics, Budapest, Hungary
X Li China Institute of Atomic Energy, Beijing, China
X L Li Central China Normal University, Wuhan, China
J Lien University of South-Eastern Norway, Kongsberg, Norway
R Lietava School of Physics and Astronomy, University of Birmingham, Birmingham, United Kingdom
B Lim Department of Physics, Pusan National University, Pusan, Republic of Korea Dipartimento di Fisica dell'Università and Sezione INFN, Turin, Italy
S H Lim Department of Physics, Pusan National University, Pusan, Republic of Korea
V Lindenstruth Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
A Lindner Horia Hulubei National Institute of Physics and Nuclear Engineering, Bucharest, Romania
C Lippmann Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
A Liu Department of Physics, University of California, Berkeley, California, USA
D H Liu Central China Normal University, Wuhan, China
J Liu University of Liverpool, Liverpool, United Kingdom
I M Lofnes Department of Physics and Technology, University of Bergen, Bergen, Norway
C Loizides Oak Ridge National Laboratory, Oak Ridge, Tennessee, USA
S Lokos The Henryk Niewodniczanski Institute of Nuclear Physics, Polish Academy of Sciences, Cracow, Poland
P Loncar Faculty of Electrical Engineering, Mechanical Engineering and Naval Architecture, University of Split, Split, Croatia
J A Lopez Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
X Lopez Université Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France
E López Torres Centro de Aplicaciones Tecnológicas y Desarrollo Nuclear (CEADEN), Havana, Cuba
P Lu Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany University of Science and Technology of China, Hefei, China
J R Luhder Westfälische Wilhelms-Universität Münster, Institut für Kernphysik, Munster, Germany
M Lunardon Dipartimento di Fisica e Astronomia dell'Università and Sezione INFN, Padova, Italy
G Luparello INFN, Sezione di Trieste, Trieste, Italy
Y G Ma Fudan University, Shanghai, China
A Maevskaya Affiliated with an institute covered by a cooperation agreement with CERN
M Mager European Organization for Nuclear Research (CERN), Geneva, Switzerland
T Mahmoud Helmholtz-Institut für Strahlen- und Kernphysik, Rheinische Friedrich-Wilhelms-Universität Bonn, Bonn, Germany
A Maire Université de Strasbourg, CNRS, IPHC UMR 7178, F-67000 Strasbourg, France, Strasbourg, France
M V Makariev Faculty of Physics, Sofia University, Sofia, Bulgaria
M Malaev Affiliated with an institute covered by a cooperation agreement with CERN
G Malfattore Dipartimento di Fisica e Astronomia dell'Università and Sezione INFN, Bologna, Italy
N M Malik Physics Department, University of Jammu, Jammu, India
Q W Malik Department of Physics, University of Oslo, Oslo, Norway
S K Malik Physics Department, University of Jammu, Jammu, India
L Malinina Affiliated with an international laboratory covered by a cooperation agreement with CERN
D Mal'Kevich Affiliated with an institute covered by a cooperation agreement with CERN
D Mallick National Institute of Science Education and Research, Homi Bhabha National Institute, Jatni, India
N Mallick Indian Institute of Technology Indore, Indore, India
G Mandaglio Dipartimento di Scienze MIFT, Università di Messina, Messina, Italy INFN, Sezione di Catania, Catania, Italy
V Manko Affiliated with an institute covered by a cooperation agreement with CERN
F Manso Université Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France
V Manzari INFN, Sezione di Bari, Bari, Italy
Y Mao Central China Normal University, Wuhan, China
G V Margagliotti Dipartimento di Fisica dell'Università and Sezione INFN, Trieste, Italy
A Margotti INFN, Sezione di Bologna, Bologna, Italy
A Marín Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
C Markert The University of Texas at Austin, Austin, Texas, USA
P Martinengo European Organization for Nuclear Research (CERN), Geneva, Switzerland
J L Martinez University of Houston, Houston, Texas, USA
M I Martínez High Energy Physics Group, Universidad Autónoma de Puebla, Puebla, Mexico
G Martínez García SUBATECH, IMT Atlantique, Nantes Université, CNRS-IN2P3, Nantes, France
S Masciocchi Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
M Masera Dipartimento di Fisica dell'Università and Sezione INFN, Turin, Italy
A Masoni INFN, Sezione di Cagliari, Cagliari, Italy
L Massacrier Laboratoire de Physique des 2 Infinis, Irène Joliot-Curie, Orsay, France
A Mastroserio INFN, Sezione di Bari, Bari, Italy Università degli Studi di Foggia, Foggia, Italy
A M Mathis Physik Department, Technische Universität München, Munich, Germany
O Matonoha Lund University Department of Physics, Division of Particle Physics, Lund, Sweden
P F T Matuoka Universidade de São Paulo (USP), São Paulo, Brazil
A Matyja The Henryk Niewodniczanski Institute of Nuclear Physics, Polish Academy of Sciences, Cracow, Poland
C Mayer The Henryk Niewodniczanski Institute of Nuclear Physics, Polish Academy of Sciences, Cracow, Poland
A L Mazuecos European Organization for Nuclear Research (CERN), Geneva, Switzerland
F Mazzaschi Dipartimento di Fisica dell'Università and Sezione INFN, Turin, Italy
M Mazzilli European Organization for Nuclear Research (CERN), Geneva, Switzerland
J E Mdhluli University of the Witwatersrand, Johannesburg, South Africa
A F Mechler Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
Y Melikyan Helsinki Institute of Physics (HIP), Helsinki, Finland Affiliated with an institute covered by a cooperation agreement with CERN
A Menchaca-Rocha Instituto de Física, Universidad Nacional Autónoma de México, Mexico City, Mexico
E Meninno Dipartimento di Fisica 'E.R. Caianiello' dell' Università and Gruppo Collegato INFN, Salerno, Italy Stefan Meyer Institut für Subatomare Physik (SMI), Vienna, Austria
A S Menon University of Houston, Houston, Texas, USA
M Meres Comenius University Bratislava, Faculty of Mathematics, Physics and Informatics, Bratislava, Slovak Republic
S Mhlanga iThemba LABS, National Research Foundation, Somerset West, South Africa University of Cape Town, Cape Town, South Africa
Y Miake University of Tsukuba, Tsukuba, Japan
L Micheletti INFN, Sezione di Torino, Turin, Italy
L C Migliorin Université de Lyon, CNRS/IN2P3, Institut de Physique des 2 Infinis de Lyon, Lyon, France
D L Mihaylov Physik Department, Technische Universität München, Munich, Germany
K Mikhaylov Affiliated with an institute covered by a cooperation agreement with CERN Affiliated with an international laboratory covered by a cooperation agreement with CERN
A N Mishra Wigner Research Centre for Physics, Budapest, Hungary
D Miśkowiec Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
A Modak Bose Institute, Department of Physics, and Centre for Astroparticle Physics and Space Science (CAPSS), Kolkata, India
A P Mohanty Institute for Gravitational and Subatomic Physics (GRASP), Utrecht University/Nikhef, Utrecht, Netherlands
B Mohanty National Institute of Science Education and Research, Homi Bhabha National Institute, Jatni, India
M Mohisin Khan Department of Physics, Aligarh Muslim University, Aligarh, India
M A Molander Helsinki Institute of Physics (HIP), Helsinki, Finland
Z Moravcova Niels Bohr Institute, University of Copenhagen, Copenhagen, Denmark
C Mordasini Physik Department, Technische Universität München, Munich, Germany
D A Moreira De Godoy Westfälische Wilhelms-Universität Münster, Institut für Kernphysik, Munster, Germany
I Morozov Affiliated with an institute covered by a cooperation agreement with CERN
A Morsch European Organization for Nuclear Research (CERN), Geneva, Switzerland
T Mrnjavac European Organization for Nuclear Research (CERN), Geneva, Switzerland
V Muccifora INFN, Laboratori Nazionali di Frascati, Frascati, Italy
S Muhuri Variable Energy Cyclotron Centre, Homi Bhabha National Institute, Kolkata, India
J D Mulligan Lawrence Berkeley National Laboratory, Berkeley, California, USA
A Mulliri Dipartimento di Fisica dell'Università and Sezione INFN, Cagliari, Italy
M G Munhoz Universidade de São Paulo (USP), São Paulo, Brazil
R H Munzer Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
H Murakami University of Tokyo, Tokyo, Japan
S Murray University of Cape Town, Cape Town, South Africa
L Musa European Organization for Nuclear Research (CERN), Geneva, Switzerland
J Musinsky Institute of Experimental Physics, Slovak Academy of Sciences, Košice, Slovak Republic
J W Myrcha Warsaw University of Technology, Warsaw, Poland
B Naik University of the Witwatersrand, Johannesburg, South Africa
A I Nambrath Department of Physics, University of California, Berkeley, California, USA
B K Nandi Indian Institute of Technology Bombay (IIT), Mumbai, India
R Nania INFN, Sezione di Bologna, Bologna, Italy
E Nappi INFN, Sezione di Bari, Bari, Italy
A F Nassirpour Lund University Department of Physics, Division of Particle Physics, Lund, Sweden
A Nath Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
C Nattrass University of Tennessee, Knoxville, Tennessee, USA
M N Naydenov Faculty of Physics, Sofia University, Sofia, Bulgaria
A Neagu Department of Physics, University of Oslo, Oslo, Norway
A Negru University Politehnica of Bucharest, Bucharest, Romania
L Nellen Instituto de Ciencias Nucleares, Universidad Nacional Autónoma de México, Mexico City, Mexico
S V Nesbo Faculty of Engineering and Science, Western Norway University of Applied Sciences, Bergen, Norway
G Neskovic Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
D Nesterov Affiliated with an institute covered by a cooperation agreement with CERN
B S Nielsen Niels Bohr Institute, University of Copenhagen, Copenhagen, Denmark
E G Nielsen Niels Bohr Institute, University of Copenhagen, Copenhagen, Denmark
S Nikolaev Affiliated with an institute covered by a cooperation agreement with CERN
S Nikulin Affiliated with an institute covered by a cooperation agreement with CERN
V Nikulin Affiliated with an institute covered by a cooperation agreement with CERN
F Noferini INFN, Sezione di Bologna, Bologna, Italy
S Noh Chungbuk National University, Cheongju, Republic of Korea
P Nomokonov Affiliated with an international laboratory covered by a cooperation agreement with CERN
J Norman University of Liverpool, Liverpool, United Kingdom
N Novitzky University of Tsukuba, Tsukuba, Japan
P Nowakowski Warsaw University of Technology, Warsaw, Poland
A Nyanin Affiliated with an institute covered by a cooperation agreement with CERN
J Nystrand Department of Physics and Technology, University of Bergen, Bergen, Norway
M Ogino Nagasaki Institute of Applied Science, Nagasaki, Japan
A Ohlson Lund University Department of Physics, Division of Particle Physics, Lund, Sweden
V A Okorokov Affiliated with an institute covered by a cooperation agreement with CERN
J Oleniacz Warsaw University of Technology, Warsaw, Poland
A C Oliveira Da Silva University of Tennessee, Knoxville, Tennessee, USA
M H Oliver Yale University, New Haven, Connecticut, USA
A Onnerstad University of Jyväskylä, Jyväskylä, Finland
C Oppedisano INFN, Sezione di Torino, Turin, Italy
A Ortiz Velasquez Instituto de Ciencias Nucleares, Universidad Nacional Autónoma de México, Mexico City, Mexico
J Otwinowski The Henryk Niewodniczanski Institute of Nuclear Physics, Polish Academy of Sciences, Cracow, Poland
M Oya Physics Program and International Institute for Sustainability with Knotted Chiral Meta Matter (SKCM2), Hiroshima University, Hiroshima, Japan
K Oyama Nagasaki Institute of Applied Science, Nagasaki, Japan
Y Pachmayer Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
S Padhan Indian Institute of Technology Bombay (IIT), Mumbai, India
D Pagano INFN, Sezione di Pavia, Pavia, Italy Università di Brescia, Brescia, Italy
G Paić Instituto de Ciencias Nucleares, Universidad Nacional Autónoma de México, Mexico City, Mexico
A Palasciano INFN, Sezione di Bari, Bari, Italy
S Panebianco Université Paris-Saclay Centre d'Etudes de Saclay (CEA), IRFU, Départment de Physique Nucléaire (DPhN), Saclay, France
H Park University of Tsukuba, Tsukuba, Japan
H Park Sungkyunkwan University, Suwon City, Republic of Korea
J Park Inha University, Incheon, Republic of Korea
J E Parkkila European Organization for Nuclear Research (CERN), Geneva, Switzerland
R N Patra Physics Department, University of Jammu, Jammu, India
B Paul Dipartimento di Fisica dell'Università and Sezione INFN, Cagliari, Italy
H Pei Central China Normal University, Wuhan, China
T Peitzmann Institute for Gravitational and Subatomic Physics (GRASP), Utrecht University/Nikhef, Utrecht, Netherlands
X Peng Central China Normal University, Wuhan, China
M Pennisi Dipartimento di Fisica dell'Università and Sezione INFN, Turin, Italy
L G Pereira Instituto de Física, Universidade Federal do Rio Grande do Sul (UFRGS), Porto Alegre, Brazil
D Peresunko Affiliated with an institute covered by a cooperation agreement with CERN
G M Perez Centro de Aplicaciones Tecnológicas y Desarrollo Nuclear (CEADEN), Havana, Cuba
S Perrin Université Paris-Saclay Centre d'Etudes de Saclay (CEA), IRFU, Départment de Physique Nucléaire (DPhN), Saclay, France
Y Pestov Affiliated with an institute covered by a cooperation agreement with CERN
V Petráček Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic
V Petrov Affiliated with an institute covered by a cooperation agreement with CERN
M Petrovici Horia Hulubei National Institute of Physics and Nuclear Engineering, Bucharest, Romania
R P Pezzi Instituto de Física, Universidade Federal do Rio Grande do Sul (UFRGS), Porto Alegre, Brazil SUBATECH, IMT Atlantique, Nantes Université, CNRS-IN2P3, Nantes, France
S Piano INFN, Sezione di Trieste, Trieste, Italy
M Pikna Comenius University Bratislava, Faculty of Mathematics, Physics and Informatics, Bratislava, Slovak Republic
P Pillot SUBATECH, IMT Atlantique, Nantes Université, CNRS-IN2P3, Nantes, France
O Pinazza European Organization for Nuclear Research (CERN), Geneva, Switzerland INFN, Sezione di Bologna, Bologna, Italy
L Pinsky University of Houston, Houston, Texas, USA
C Pinto Physik Department, Technische Universität München, Munich, Germany
S Pisano INFN, Laboratori Nazionali di Frascati, Frascati, Italy
M Płoskoń Lawrence Berkeley National Laboratory, Berkeley, California, USA
M Planinic Physics department, Faculty of science, University of Zagreb, Zagreb, Croatia
F Pliquett Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
M G Poghosyan Oak Ridge National Laboratory, Oak Ridge, Tennessee, USA
B Polichtchouk Affiliated with an institute covered by a cooperation agreement with CERN
S Politano Dipartimento DISAT del Politecnico and Sezione INFN, Turin, Italy
N Poljak Physics department, Faculty of science, University of Zagreb, Zagreb, Croatia
A Pop Horia Hulubei National Institute of Physics and Nuclear Engineering, Bucharest, Romania
S Porteboeuf-Houssais Université Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France
V Pozdniakov Affiliated with an international laboratory covered by a cooperation agreement with CERN
K K Pradhan Indian Institute of Technology Indore, Indore, India
S K Prasad Bose Institute, Department of Physics, and Centre for Astroparticle Physics and Space Science (CAPSS), Kolkata, India
S Prasad Indian Institute of Technology Indore, Indore, India
R Preghenella INFN, Sezione di Bologna, Bologna, Italy
F Prino INFN, Sezione di Torino, Turin, Italy
C A Pruneau Wayne State University, Detroit, Michigan, USA
I Pshenichnov Affiliated with an institute covered by a cooperation agreement with CERN
M Puccio European Organization for Nuclear Research (CERN), Geneva, Switzerland
S Pucillo Dipartimento di Fisica dell'Università and Sezione INFN, Turin, Italy
Z Pugelova Technical University of Košice, Košice, Slovak Republic
S Qiu Nikhef, National institute for subatomic physics, Amsterdam, Netherlands
L Quaglia Dipartimento di Fisica dell'Università and Sezione INFN, Turin, Italy
R E Quishpe University of Houston, Houston, Texas, USA
S Ragoni Creighton University, Omaha, Nebraska, USA School of Physics and Astronomy, University of Birmingham, Birmingham, United Kingdom
A Rakotozafindrabe Université Paris-Saclay Centre d'Etudes de Saclay (CEA), IRFU, Départment de Physique Nucléaire (DPhN), Saclay, France
L Ramello INFN, Sezione di Torino, Turin, Italy Università del Piemonte Orientale, Vercelli, Italy
F Rami Université de Strasbourg, CNRS, IPHC UMR 7178, F-67000 Strasbourg, France, Strasbourg, France
S A R Ramirez High Energy Physics Group, Universidad Autónoma de Puebla, Puebla, Mexico
T A Rancien Laboratoire de Physique Subatomique et de Cosmologie, Université Grenoble-Alpes, CNRS-IN2P3, Grenoble, France
M Rasa Dipartimento di Fisica e Astronomia dell'Università and Sezione INFN, Catania, Italy
S S Räsänen Helsinki Institute of Physics (HIP), Helsinki, Finland
R Rath Indian Institute of Technology Indore, Indore, India INFN, Sezione di Bologna, Bologna, Italy
M P Rauch Department of Physics and Technology, University of Bergen, Bergen, Norway
I Ravasenga Nikhef, National institute for subatomic physics, Amsterdam, Netherlands
K F Read Oak Ridge National Laboratory, Oak Ridge, Tennessee, USA University of Tennessee, Knoxville, Tennessee, USA
C Reckziegel Universidade Federal do ABC, Santo Andre, Brazil
A R Redelbach Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
K Redlich National Centre for Nuclear Research, Warsaw, Poland
A Rehman Department of Physics and Technology, University of Bergen, Bergen, Norway
F Reidt European Organization for Nuclear Research (CERN), Geneva, Switzerland
H A Reme-Ness Faculty of Engineering and Science, Western Norway University of Applied Sciences, Bergen, Norway
Z Rescakova Faculty of Science, P.J. Šafárik University, Košice, Slovak Republic
K Reygers Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
A Riabov Affiliated with an institute covered by a cooperation agreement with CERN
V Riabov Affiliated with an institute covered by a cooperation agreement with CERN
R Ricci Dipartimento di Fisica 'E.R. Caianiello' dell' Università and Gruppo Collegato INFN, Salerno, Italy
M Richter Department of Physics, University of Oslo, Oslo, Norway
A A Riedel Physik Department, Technische Universität München, Munich, Germany
W Riegler European Organization for Nuclear Research (CERN), Geneva, Switzerland
C Ristea Institute of Space Science (ISS), Bucharest, Romania
M Rodríguez Cahuantzi High Energy Physics Group, Universidad Autónoma de Puebla, Puebla, Mexico
K Røed Department of Physics, University of Oslo, Oslo, Norway
R Rogalev Affiliated with an institute covered by a cooperation agreement with CERN
E Rogochaya Affiliated with an international laboratory covered by a cooperation agreement with CERN
T S Rogoschinski Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
D Rohr European Organization for Nuclear Research (CERN), Geneva, Switzerland
D Röhrich Department of Physics and Technology, University of Bergen, Bergen, Norway
P F Rojas High Energy Physics Group, Universidad Autónoma de Puebla, Puebla, Mexico
S Rojas Torres Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic
P S Rokita Warsaw University of Technology, Warsaw, Poland
G Romanenko Affiliated with an international laboratory covered by a cooperation agreement with CERN
F Ronchetti INFN, Laboratori Nazionali di Frascati, Frascati, Italy
A Rosano Dipartimento di Scienze MIFT, Università di Messina, Messina, Italy INFN, Sezione di Catania, Catania, Italy
E D Rosas Instituto de Ciencias Nucleares, Universidad Nacional Autónoma de México, Mexico City, Mexico
A Rossi INFN, Sezione di Padova, Padova, Italy
A Roy Indian Institute of Technology Indore, Indore, India
S Roy Indian Institute of Technology Bombay (IIT), Mumbai, India
N Rubini Dipartimento di Fisica e Astronomia dell'Università and Sezione INFN, Bologna, Italy
O V Rueda Lund University Department of Physics, Division of Particle Physics, Lund, Sweden University of Houston, Houston, Texas, USA
D Ruggiano Warsaw University of Technology, Warsaw, Poland
R Rui Dipartimento di Fisica dell'Università and Sezione INFN, Trieste, Italy
B Rumyantsev Affiliated with an international laboratory covered by a cooperation agreement with CERN
P G Russek AGH University of Science and Technology, Cracow, Poland
R Russo Nikhef, National institute for subatomic physics, Amsterdam, Netherlands
A Rustamov National Nuclear Research Center, Baku, Azerbaijan
E Ryabinkin Affiliated with an institute covered by a cooperation agreement with CERN
Y Ryabov Affiliated with an institute covered by a cooperation agreement with CERN
A Rybicki The Henryk Niewodniczanski Institute of Nuclear Physics, Polish Academy of Sciences, Cracow, Poland
H Rytkonen University of Jyväskylä, Jyväskylä, Finland
W Rzesa Warsaw University of Technology, Warsaw, Poland
O A M Saarimaki Helsinki Institute of Physics (HIP), Helsinki, Finland
R Sadek SUBATECH, IMT Atlantique, Nantes Université, CNRS-IN2P3, Nantes, France
S Sadhu Dipartimento Interateneo di Fisica 'M. Merlin' and Sezione INFN, Bari, Italy
S Sadovsky Affiliated with an institute covered by a cooperation agreement with CERN
J Saetre Department of Physics and Technology, University of Bergen, Bergen, Norway
K Šafařík Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic
S K Saha Bose Institute, Department of Physics, and Centre for Astroparticle Physics and Space Science (CAPSS), Kolkata, India
S Saha National Institute of Science Education and Research, Homi Bhabha National Institute, Jatni, India
B Sahoo Indian Institute of Technology Bombay (IIT), Mumbai, India
R Sahoo Indian Institute of Technology Indore, Indore, India
S Sahoo Institute of Physics, Homi Bhabha National Institute, Bhubaneswar, India
D Sahu Indian Institute of Technology Indore, Indore, India
P K Sahu Institute of Physics, Homi Bhabha National Institute, Bhubaneswar, India
J Saini Variable Energy Cyclotron Centre, Homi Bhabha National Institute, Kolkata, India
K Sajdakova Faculty of Science, P.J. Šafárik University, Košice, Slovak Republic
S Sakai University of Tsukuba, Tsukuba, Japan
M P Salvan Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
S Sambyal Physics Department, University of Jammu, Jammu, India
I Sanna European Organization for Nuclear Research (CERN), Geneva, Switzerland Physik Department, Technische Universität München, Munich, Germany
T B Saramela Universidade de São Paulo (USP), São Paulo, Brazil
D Sarkar Wayne State University, Detroit, Michigan, USA
N Sarkar Variable Energy Cyclotron Centre, Homi Bhabha National Institute, Kolkata, India
P Sarma Gauhati University, Department of Physics, Guwahati, India
V Sarritzu Dipartimento di Fisica dell'Università and Sezione INFN, Cagliari, Italy
V M Sarti Physik Department, Technische Universität München, Munich, Germany
M H P Sas Yale University, New Haven, Connecticut, USA
J Schambach Oak Ridge National Laboratory, Oak Ridge, Tennessee, USA
H S Scheid Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
C Schiaua Horia Hulubei National Institute of Physics and Nuclear Engineering, Bucharest, Romania
R Schicker Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
A Schmah Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
C Schmidt Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
H R Schmidt Physikalisches Institut, Eberhard-Karls-Universität Tübingen, Tubingen, Germany
M O Schmidt European Organization for Nuclear Research (CERN), Geneva, Switzerland
M Schmidt Physikalisches Institut, Eberhard-Karls-Universität Tübingen, Tubingen, Germany
N V Schmidt Oak Ridge National Laboratory, Oak Ridge, Tennessee, USA
A R Schmier University of Tennessee, Knoxville, Tennessee, USA
R Schotter Université de Strasbourg, CNRS, IPHC UMR 7178, F-67000 Strasbourg, France, Strasbourg, France
A Schröter Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
J Schukraft European Organization for Nuclear Research (CERN), Geneva, Switzerland
K Schwarz Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
K Schweda Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
G Scioli Dipartimento di Fisica e Astronomia dell'Università and Sezione INFN, Bologna, Italy
E Scomparin INFN, Sezione di Torino, Turin, Italy
J E Seger Creighton University, Omaha, Nebraska, USA
Y Sekiguchi University of Tokyo, Tokyo, Japan
D Sekihata University of Tokyo, Tokyo, Japan
I Selyuzhenkov Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany Affiliated with an institute covered by a cooperation agreement with CERN
S Senyukov Université de Strasbourg, CNRS, IPHC UMR 7178, F-67000 Strasbourg, France, Strasbourg, France
J J Seo Inha University, Incheon, Republic of Korea
D Serebryakov Affiliated with an institute covered by a cooperation agreement with CERN
L Šerkšnytė Physik Department, Technische Universität München, Munich, Germany
A Sevcenco Institute of Space Science (ISS), Bucharest, Romania
T J Shaba iThemba LABS, National Research Foundation, Somerset West, South Africa
A Shabetai SUBATECH, IMT Atlantique, Nantes Université, CNRS-IN2P3, Nantes, France
R Shahoyan European Organization for Nuclear Research (CERN), Geneva, Switzerland
A Shangaraev Affiliated with an institute covered by a cooperation agreement with CERN
A Sharma Physics Department, Panjab University, Chandigarh, India
D Sharma Indian Institute of Technology Bombay (IIT), Mumbai, India
H Sharma The Henryk Niewodniczanski Institute of Nuclear Physics, Polish Academy of Sciences, Cracow, Poland
M Sharma Physics Department, University of Jammu, Jammu, India
S Sharma Nagasaki Institute of Applied Science, Nagasaki, Japan
S Sharma Physics Department, University of Jammu, Jammu, India
U Sharma Physics Department, University of Jammu, Jammu, India
A Shatat Laboratoire de Physique des 2 Infinis, Irène Joliot-Curie, Orsay, France
O Sheibani University of Houston, Houston, Texas, USA
K Shigaki Physics Program and International Institute for Sustainability with Knotted Chiral Meta Matter (SKCM2), Hiroshima University, Hiroshima, Japan
M Shimomura Nara Women's University (NWU), Nara, Japan
J Shin Chungbuk National University, Cheongju, Republic of Korea
S Shirinkin Affiliated with an institute covered by a cooperation agreement with CERN
Q Shou Fudan University, Shanghai, China
Y Sibiriak Affiliated with an institute covered by a cooperation agreement with CERN
S Siddhanta INFN, Sezione di Cagliari, Cagliari, Italy
T Siemiarczuk National Centre for Nuclear Research, Warsaw, Poland
T F Silva Universidade de São Paulo (USP), São Paulo, Brazil
D Silvermyr Lund University Department of Physics, Division of Particle Physics, Lund, Sweden
T Simantathammakul Suranaree University of Technology, Nakhon Ratchasima, Thailand
R Simeonov Faculty of Physics, Sofia University, Sofia, Bulgaria
B Singh Physics Department, University of Jammu, Jammu, India
B Singh Physik Department, Technische Universität München, Munich, Germany
R Singh National Institute of Science Education and Research, Homi Bhabha National Institute, Jatni, India
R Singh Physics Department, University of Jammu, Jammu, India
R Singh Indian Institute of Technology Indore, Indore, India
S Singh Department of Physics, Aligarh Muslim University, Aligarh, India
V K Singh Variable Energy Cyclotron Centre, Homi Bhabha National Institute, Kolkata, India
V Singhal Variable Energy Cyclotron Centre, Homi Bhabha National Institute, Kolkata, India
T Sinha Saha Institute of Nuclear Physics, Homi Bhabha National Institute, Kolkata, India
B Sitar Comenius University Bratislava, Faculty of Mathematics, Physics and Informatics, Bratislava, Slovak Republic
M Sitta INFN, Sezione di Torino, Turin, Italy Università del Piemonte Orientale, Vercelli, Italy
T B Skaali Department of Physics, University of Oslo, Oslo, Norway
G Skorodumovs Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
M Slupecki Helsinki Institute of Physics (HIP), Helsinki, Finland
N Smirnov Yale University, New Haven, Connecticut, USA
R J M Snellings Institute for Gravitational and Subatomic Physics (GRASP), Utrecht University/Nikhef, Utrecht, Netherlands
E H Solheim Department of Physics, University of Oslo, Oslo, Norway
J Song University of Houston, Houston, Texas, USA
A Songmoolnak Suranaree University of Technology, Nakhon Ratchasima, Thailand
F Soramel Dipartimento di Fisica e Astronomia dell'Università and Sezione INFN, Padova, Italy
R Spijkers Nikhef, National institute for subatomic physics, Amsterdam, Netherlands
I Sputowska The Henryk Niewodniczanski Institute of Nuclear Physics, Polish Academy of Sciences, Cracow, Poland
J Staa Lund University Department of Physics, Division of Particle Physics, Lund, Sweden
J Stachel Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
I Stan Institute of Space Science (ISS), Bucharest, Romania
P J Steffanic University of Tennessee, Knoxville, Tennessee, USA
S F Stiefelmaier Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
D Stocco SUBATECH, IMT Atlantique, Nantes Université, CNRS-IN2P3, Nantes, France
I Storehaug Department of Physics, University of Oslo, Oslo, Norway
P Stratmann Westfälische Wilhelms-Universität Münster, Institut für Kernphysik, Munster, Germany
S Strazzi Dipartimento di Fisica e Astronomia dell'Università and Sezione INFN, Bologna, Italy
C P Stylianidis Nikhef, National institute for subatomic physics, Amsterdam, Netherlands
A A P Suaide Universidade de São Paulo (USP), São Paulo, Brazil
C Suire Laboratoire de Physique des 2 Infinis, Irène Joliot-Curie, Orsay, France
M Sukhanov Affiliated with an institute covered by a cooperation agreement with CERN
M Suljic European Organization for Nuclear Research (CERN), Geneva, Switzerland
R Sultanov Affiliated with an institute covered by a cooperation agreement with CERN
V Sumberia Physics Department, University of Jammu, Jammu, India
S Sumowidagdo National Research and Innovation Agency - BRIN, Jakarta, Indonesia
S Swain Institute of Physics, Homi Bhabha National Institute, Bhubaneswar, India
I Szarka Comenius University Bratislava, Faculty of Mathematics, Physics and Informatics, Bratislava, Slovak Republic
S F Taghavi Physik Department, Technische Universität München, Munich, Germany
G Taillepied Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
J Takahashi Universidade Estadual de Campinas (UNICAMP), Campinas, Brazil
G J Tambave Department of Physics and Technology, University of Bergen, Bergen, Norway
S Tang Central China Normal University, Wuhan, China Université Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France
Z Tang University of Science and Technology of China, Hefei, China
J D Tapia Takaki University of Kansas, Lawrence, Kansas, USA
N Tapus University Politehnica of Bucharest, Bucharest, Romania
L A Tarasovicova Westfälische Wilhelms-Universität Münster, Institut für Kernphysik, Munster, Germany
M G Tarzila Horia Hulubei National Institute of Physics and Nuclear Engineering, Bucharest, Romania
G F Tassielli Dipartimento Interateneo di Fisica 'M. Merlin' and Sezione INFN, Bari, Italy
A Tauro European Organization for Nuclear Research (CERN), Geneva, Switzerland
G Tejeda Muñoz High Energy Physics Group, Universidad Autónoma de Puebla, Puebla, Mexico
A Telesca European Organization for Nuclear Research (CERN), Geneva, Switzerland
L Terlizzi Dipartimento di Fisica dell'Università and Sezione INFN, Turin, Italy
C Terrevoli University of Houston, Houston, Texas, USA
G Tersimonov Bogolyubov Institute for Theoretical Physics, National Academy of Sciences of Ukraine, Kiev, Ukraine
S Thakur Bose Institute, Department of Physics, and Centre for Astroparticle Physics and Space Science (CAPSS), Kolkata, India
D Thomas The University of Texas at Austin, Austin, Texas, USA
A Tikhonov Affiliated with an institute covered by a cooperation agreement with CERN
A R Timmins University of Houston, Houston, Texas, USA
M Tkacik Technical University of Košice, Košice, Slovak Republic
T Tkacik Technical University of Košice, Košice, Slovak Republic
A Toia Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
R Tokumoto Physics Program and International Institute for Sustainability with Knotted Chiral Meta Matter (SKCM2), Hiroshima University, Hiroshima, Japan
N Topilskaya Affiliated with an institute covered by a cooperation agreement with CERN
M Toppi INFN, Laboratori Nazionali di Frascati, Frascati, Italy
F Torales-Acosta Department of Physics, University of California, Berkeley, California, USA
T Tork Laboratoire de Physique des 2 Infinis, Irène Joliot-Curie, Orsay, France
A G Torres Ramos Dipartimento Interateneo di Fisica 'M. Merlin' and Sezione INFN, Bari, Italy
A Trifiró Dipartimento di Scienze MIFT, Università di Messina, Messina, Italy INFN, Sezione di Catania, Catania, Italy
A S Triolo Dipartimento di Scienze MIFT, Università di Messina, Messina, Italy INFN, Sezione di Catania, Catania, Italy
S Tripathy INFN, Sezione di Bologna, Bologna, Italy
T Tripathy Indian Institute of Technology Bombay (IIT), Mumbai, India
S Trogolo European Organization for Nuclear Research (CERN), Geneva, Switzerland
V Trubnikov Bogolyubov Institute for Theoretical Physics, National Academy of Sciences of Ukraine, Kiev, Ukraine
W H Trzaska University of Jyväskylä, Jyväskylä, Finland
T P Trzcinski Warsaw University of Technology, Warsaw, Poland
A Tumkin Affiliated with an institute covered by a cooperation agreement with CERN
R Turrisi INFN, Sezione di Padova, Padova, Italy
T S Tveter Department of Physics, University of Oslo, Oslo, Norway
K Ullaland Department of Physics and Technology, University of Bergen, Bergen, Norway
B Ulukutlu Physik Department, Technische Universität München, Munich, Germany
A Uras Université de Lyon, CNRS/IN2P3, Institut de Physique des 2 Infinis de Lyon, Lyon, France
M Urioni INFN, Sezione di Pavia, Pavia, Italy Università di Brescia, Brescia, Italy
G L Usai Dipartimento di Fisica dell'Università and Sezione INFN, Cagliari, Italy
M Vala Faculty of Science, P.J. Šafárik University, Košice, Slovak Republic
N Valle Dipartimento di Fisica, Università di Pavia, Pavia, Italy
L V R van Doremalen Institute for Gravitational and Subatomic Physics (GRASP), Utrecht University/Nikhef, Utrecht, Netherlands
M van Leeuwen Nikhef, National institute for subatomic physics, Amsterdam, Netherlands
C A van Veen Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
R J G van Weelden Nikhef, National institute for subatomic physics, Amsterdam, Netherlands
P Vande Vyvre European Organization for Nuclear Research (CERN), Geneva, Switzerland
D Varga Wigner Research Centre for Physics, Budapest, Hungary
Z Varga Wigner Research Centre for Physics, Budapest, Hungary
M Vasileiou National and Kapodistrian University of Athens, School of Science, Department of Physics, Athens, Greece
A Vasiliev Affiliated with an institute covered by a cooperation agreement with CERN
O Vázquez Doce INFN, Laboratori Nazionali di Frascati, Frascati, Italy
V Vechernin Affiliated with an institute covered by a cooperation agreement with CERN
E Vercellin Dipartimento di Fisica dell'Università and Sezione INFN, Turin, Italy
S Vergara Limón High Energy Physics Group, Universidad Autónoma de Puebla, Puebla, Mexico
L Vermunt Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
R Vértesi Wigner Research Centre for Physics, Budapest, Hungary
M Verweij Institute for Gravitational and Subatomic Physics (GRASP), Utrecht University/Nikhef, Utrecht, Netherlands
L Vickovic Faculty of Electrical Engineering, Mechanical Engineering and Naval Architecture, University of Split, Split, Croatia
Z Vilakazi University of the Witwatersrand, Johannesburg, South Africa
O Villalobos Baillie School of Physics and Astronomy, University of Birmingham, Birmingham, United Kingdom
G Vino INFN, Sezione di Bari, Bari, Italy
A Vinogradov Affiliated with an institute covered by a cooperation agreement with CERN
T Virgili Dipartimento di Fisica 'E.R. Caianiello' dell' Università and Gruppo Collegato INFN, Salerno, Italy
V Vislavicius Niels Bohr Institute, University of Copenhagen, Copenhagen, Denmark
A Vodopyanov Affiliated with an international laboratory covered by a cooperation agreement with CERN
B Volkel European Organization for Nuclear Research (CERN), Geneva, Switzerland
M A Völkl Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
K Voloshin Affiliated with an institute covered by a cooperation agreement with CERN
S A Voloshin Wayne State University, Detroit, Michigan, USA
G Volpe Dipartimento Interateneo di Fisica 'M. Merlin' and Sezione INFN, Bari, Italy
B von Haller European Organization for Nuclear Research (CERN), Geneva, Switzerland
I Vorobyev Physik Department, Technische Universität München, Munich, Germany
N Vozniuk Affiliated with an institute covered by a cooperation agreement with CERN
J Vrláková Faculty of Science, P.J. Šafárik University, Košice, Slovak Republic
C Wang Fudan University, Shanghai, China
D Wang Fudan University, Shanghai, China
Y Wang Fudan University, Shanghai, China
A Wegrzynek European Organization for Nuclear Research (CERN), Geneva, Switzerland
F T Weiglhofer Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
S C Wenzel European Organization for Nuclear Research (CERN), Geneva, Switzerland
J P Wessels Westfälische Wilhelms-Universität Münster, Institut für Kernphysik, Munster, Germany
S L Weyhmiller Yale University, New Haven, Connecticut, USA
J Wiechula Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
J Wikne Department of Physics, University of Oslo, Oslo, Norway
G Wilk National Centre for Nuclear Research, Warsaw, Poland
J Wilkinson Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
G A Willems Westfälische Wilhelms-Universität Münster, Institut für Kernphysik, Munster, Germany
B Windelband Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
M Winn Université Paris-Saclay Centre d'Etudes de Saclay (CEA), IRFU, Départment de Physique Nucléaire (DPhN), Saclay, France
J R Wright The University of Texas at Austin, Austin, Texas, USA
W Wu Fudan University, Shanghai, China
Y Wu University of Science and Technology of China, Hefei, China
R Xu Central China Normal University, Wuhan, China
A Yadav Helmholtz-Institut für Strahlen- und Kernphysik, Rheinische Friedrich-Wilhelms-Universität Bonn, Bonn, Germany
A K Yadav Variable Energy Cyclotron Centre, Homi Bhabha National Institute, Kolkata, India
S Yalcin KTO Karatay University, Konya, Turkey
Y Yamaguchi Physics Program and International Institute for Sustainability with Knotted Chiral Meta Matter (SKCM2), Hiroshima University, Hiroshima, Japan
K Yamakawa Physics Program and International Institute for Sustainability with Knotted Chiral Meta Matter (SKCM2), Hiroshima University, Hiroshima, Japan
S Yang Department of Physics and Technology, University of Bergen, Bergen, Norway
S Yano Physics Program and International Institute for Sustainability with Knotted Chiral Meta Matter (SKCM2), Hiroshima University, Hiroshima, Japan
Z Yin Central China Normal University, Wuhan, China
I-K Yoo Department of Physics, Pusan National University, Pusan, Republic of Korea
J H Yoon Inha University, Incheon, Republic of Korea
S Yuan Department of Physics and Technology, University of Bergen, Bergen, Norway
A Yuncu Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
V Zaccolo Dipartimento di Fisica dell'Università and Sezione INFN, Trieste, Italy
C Zampolli European Organization for Nuclear Research (CERN), Geneva, Switzerland
F Zanone Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
N Zardoshti European Organization for Nuclear Research (CERN), Geneva, Switzerland School of Physics and Astronomy, University of Birmingham, Birmingham, United Kingdom
A Zarochentsev Affiliated with an institute covered by a cooperation agreement with CERN
P Závada Institute of Physics of the Czech Academy of Sciences, Prague, Czech Republic
N Zaviyalov Affiliated with an institute covered by a cooperation agreement with CERN
M Zhalov Affiliated with an institute covered by a cooperation agreement with CERN
B Zhang Central China Normal University, Wuhan, China
L Zhang Fudan University, Shanghai, China
S Zhang Fudan University, Shanghai, China
X Zhang Central China Normal University, Wuhan, China
Y Zhang University of Science and Technology of China, Hefei, China
Z Zhang Central China Normal University, Wuhan, China
M Zhao China Institute of Atomic Energy, Beijing, China
V Zherebchevskii Affiliated with an institute covered by a cooperation agreement with CERN
Y Zhi China Institute of Atomic Energy, Beijing, China
D Zhou Central China Normal University, Wuhan, China
Y Zhou Niels Bohr Institute, University of Copenhagen, Copenhagen, Denmark
J Zhu Central China Normal University, Wuhan, China Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
Y Zhu Central China Normal University, Wuhan, China
S C Zugravel INFN, Sezione di Torino, Turin, Italy
N Zurlo INFN, Sezione di Pavia, Pavia, Italy Università di Brescia, Brescia, Italy

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Search for Heavy Neutral Leptons in Electron-Positron and Neutral-Pion Final States with the MicroBooNE Detector

We present the first search for heavy neutral leptons (HNLs) decaying into νe^{+}e^{-} or νπ^{0} final states in a liquid-argon time projection chamber using data collected with the MicroBooNE detector. The data were recorded synchronously with the NuMI neutrino beam from Fermilab's main injector corresponding to a total exposure of 7.01×10^{20} protons on target. We set upper limits at the 90% confidence level on the mixing parameter |U_{μ4}|^{2} in the mass ranges 10≤m_{HNL}≤150  MeV for the νe^{+}e^{-} channel and 150≤m_{HNL}≤245  MeV for the νπ^{0} channel, assuming |U_{e4}|^{2}=|U_{τ4}|^{2}=0. These limits represent the most stringent constraints in the mass range 35 Collapse

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Affiliation(s)

P Abratenko Tufts University, Medford, Massachusetts 02155, USA
O Alterkait Tufts University, Medford, Massachusetts 02155, USA
D Andrade Aldana Illinois Institute of Technology (IIT), Chicago, Illinois 60616, USA
L Arellano The University of Manchester, Manchester M13 9PL, United Kingdom
J Asaadi University of Texas, Arlington, Texas 76019, USA
A Ashkenazi Tel Aviv University, Tel Aviv, Israel, 69978
S Balasubramanian Fermi National Accelerator Laboratory (FNAL), Batavia, Illinois 60510, USA
B Baller Fermi National Accelerator Laboratory (FNAL), Batavia, Illinois 60510, USA
G Barr University of Oxford, Oxford OX1 3RH, United Kingdom
D Barrow University of Oxford, Oxford OX1 3RH, United Kingdom
J Barrow Massachusetts Institute of Technology (MIT), Cambridge, Massachusetts 02139, USA Tel Aviv University, Tel Aviv, Israel, 69978
V Basque Fermi National Accelerator Laboratory (FNAL), Batavia, Illinois 60510, USA
O Benevides Rodrigues Illinois Institute of Technology (IIT), Chicago, Illinois 60616, USA
S Berkman Fermi National Accelerator Laboratory (FNAL), Batavia, Illinois 60510, USA Michigan State University, East Lansing, Michigan 48824, USA
A Bhanderi The University of Manchester, Manchester M13 9PL, United Kingdom
A Bhat University of Chicago, Chicago, Illinois 60637, USA
M Bhattacharya Fermi National Accelerator Laboratory (FNAL), Batavia, Illinois 60510, USA
M Bishai Brookhaven National Laboratory (BNL), Upton, New York 11973, USA
A Blake Lancaster University, Lancaster LA1 4YW, United Kingdom
B Bogart University of Michigan, Ann Arbor, Michigan 48109, USA
T Bolton Kansas State University (KSU), Manhattan, Kansas 66506, USA
J Y Book Harvard University, Cambridge, Massachusetts 02138, USA
M B Brunetti University of Warwick, Coventry CV4 7AL, United Kingdom
L Camilleri Columbia University, New York, New York 10027, USA
Y Cao The University of Manchester, Manchester M13 9PL, United Kingdom
D Caratelli University of California, Santa Barbara, California 93106, USA
F Cavanna Fermi National Accelerator Laboratory (FNAL), Batavia, Illinois 60510, USA
G Cerati Fermi National Accelerator Laboratory (FNAL), Batavia, Illinois 60510, USA
A Chappell University of Warwick, Coventry CV4 7AL, United Kingdom
Y Chen SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA
J M Conrad Massachusetts Institute of Technology (MIT), Cambridge, Massachusetts 02139, USA
M Convery SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA
L Cooper-Troendle University of Pittsburgh, Pittsburgh, Pennsylvania 15260, USA
J I Crespo-Anadón Centro de Investigaciones Energéticas, Medioambientales y Tecnológicas (CIEMAT), Madrid E-28040, Spain
R Cross University of Warwick, Coventry CV4 7AL, United Kingdom
M Del Tutto Fermi National Accelerator Laboratory (FNAL), Batavia, Illinois 60510, USA
S R Dennis University of Cambridge, Cambridge CB3 0HE, United Kingdom
P Detje University of Cambridge, Cambridge CB3 0HE, United Kingdom
A Devitt Lancaster University, Lancaster LA1 4YW, United Kingdom
R Diurba Universität Bern, Bern CH-3012, Switzerland
Z Djurcic Argonne National Laboratory (ANL), Lemont, Illinois 60439, USA
R Dorrill Illinois Institute of Technology (IIT), Chicago, Illinois 60616, USA
K Duffy University of Oxford, Oxford OX1 3RH, United Kingdom
S Dytman University of Pittsburgh, Pittsburgh, Pennsylvania 15260, USA
B Eberly University of Southern Maine, Portland, Maine 04104, USA
P Englezos Rutgers University, Piscataway, New Jersey 08854, USA
A Ereditato University of Chicago, Chicago, Illinois 60637, USA Fermi National Accelerator Laboratory (FNAL), Batavia, Illinois 60510, USA
J J Evans The University of Manchester, Manchester M13 9PL, United Kingdom
R Fine Los Alamos National Laboratory (LANL), Los Alamos, New Mexico 87545, USA
O G Finnerud The University of Manchester, Manchester M13 9PL, United Kingdom
W Foreman Illinois Institute of Technology (IIT), Chicago, Illinois 60616, USA
B T Fleming University of Chicago, Chicago, Illinois 60637, USA
D Franco University of Chicago, Chicago, Illinois 60637, USA
A P Furmanski University of Minnesota, Minneapolis, Minnesota 55455, USA
F Gao University of California, Santa Barbara, California 93106, USA
D Garcia-Gamez Universidad de Granada, Granada E-18071, Spain
S Gardiner Fermi National Accelerator Laboratory (FNAL), Batavia, Illinois 60510, USA
G Ge Columbia University, New York, New York 10027, USA
S Gollapinni Los Alamos National Laboratory (LANL), Los Alamos, New Mexico 87545, USA
E Gramellini The University of Manchester, Manchester M13 9PL, United Kingdom
P Green University of Oxford, Oxford OX1 3RH, United Kingdom
H Greenlee Fermi National Accelerator Laboratory (FNAL), Batavia, Illinois 60510, USA
L Gu Lancaster University, Lancaster LA1 4YW, United Kingdom
W Gu Brookhaven National Laboratory (BNL), Upton, New York 11973, USA
R Guenette The University of Manchester, Manchester M13 9PL, United Kingdom
P Guzowski The University of Manchester, Manchester M13 9PL, United Kingdom
L Hagaman University of Chicago, Chicago, Illinois 60637, USA
O Hen Massachusetts Institute of Technology (MIT), Cambridge, Massachusetts 02139, USA
C Hilgenberg University of Minnesota, Minneapolis, Minnesota 55455, USA
G A Horton-Smith Kansas State University (KSU), Manhattan, Kansas 66506, USA
Z Imani Tufts University, Medford, Massachusetts 02155, USA
B Irwin University of Minnesota, Minneapolis, Minnesota 55455, USA
M Ismail University of Pittsburgh, Pittsburgh, Pennsylvania 15260, USA
C James Fermi National Accelerator Laboratory (FNAL), Batavia, Illinois 60510, USA
X Ji Nankai University, Nankai District, Tianjin 300071, China
J H Jo Brookhaven National Laboratory (BNL), Upton, New York 11973, USA
R A Johnson University of Cincinnati, Cincinnati, Ohio 45221, USA
Y-J Jwa Columbia University, New York, New York 10027, USA
D Kalra Columbia University, New York, New York 10027, USA
N Kamp Massachusetts Institute of Technology (MIT), Cambridge, Massachusetts 02139, USA
G Karagiorgi Columbia University, New York, New York 10027, USA
W Ketchum Fermi National Accelerator Laboratory (FNAL), Batavia, Illinois 60510, USA
M Kirby Fermi National Accelerator Laboratory (FNAL), Batavia, Illinois 60510, USA
T Kobilarcik Fermi National Accelerator Laboratory (FNAL), Batavia, Illinois 60510, USA
I Kreslo Universität Bern, Bern CH-3012, Switzerland
M B Leibovitch University of California, Santa Barbara, California 93106, USA
I Lepetic Rutgers University, Piscataway, New Jersey 08854, USA
J-Y Li University of Edinburgh, Edinburgh EH9 3FD, United Kingdom
K Li Wright Laboratory, Department of Physics, Yale University, New Haven, Connecticut 06520, USA
Y Li Brookhaven National Laboratory (BNL), Upton, New York 11973, USA
K Lin Rutgers University, Piscataway, New Jersey 08854, USA
B R Littlejohn Illinois Institute of Technology (IIT), Chicago, Illinois 60616, USA
H Liu Brookhaven National Laboratory (BNL), Upton, New York 11973, USA
W C Louis Los Alamos National Laboratory (LANL), Los Alamos, New Mexico 87545, USA
X Luo University of California, Santa Barbara, California 93106, USA
C Mariani Center for Neutrino Physics, Virginia Tech, Blacksburg, Viriginia 24061, USA
D Marsden The University of Manchester, Manchester M13 9PL, United Kingdom
J Marshall University of Warwick, Coventry CV4 7AL, United Kingdom
N Martinez Kansas State University (KSU), Manhattan, Kansas 66506, USA
D A Martinez Caicedo South Dakota School of Mines and Technology (SDSMT), Rapid City, South Dakota 57701, USA
S Martynenko Brookhaven National Laboratory (BNL), Upton, New York 11973, USA
A Mastbaum Rutgers University, Piscataway, New Jersey 08854, USA
I Mawby University of Warwick, Coventry CV4 7AL, United Kingdom
N McConkey University College London, London WC1E 6BT, United Kingdom
V Meddage Kansas State University (KSU), Manhattan, Kansas 66506, USA
J Micallef Massachusetts Institute of Technology (MIT), Cambridge, Massachusetts 02139, USA Tufts University, Medford, Massachusetts 02155, USA
K Miller University of Chicago, Chicago, Illinois 60637, USA
A Mogan Colorado State University, Fort Collins, Colorado 80523, USA
T Mohayai Fermi National Accelerator Laboratory (FNAL), Batavia, Illinois 60510, USA Indiana University, Bloomington, Indiana 47405, USA
M Mooney Colorado State University, Fort Collins, Colorado 80523, USA
A F Moor University of Cambridge, Cambridge CB3 0HE, United Kingdom
C D Moore Fermi National Accelerator Laboratory (FNAL), Batavia, Illinois 60510, USA
L Mora Lepin The University of Manchester, Manchester M13 9PL, United Kingdom
M M Moudgalya The University of Manchester, Manchester M13 9PL, United Kingdom
S Mulleriababu Universität Bern, Bern CH-3012, Switzerland
D Naples University of Pittsburgh, Pittsburgh, Pennsylvania 15260, USA
A Navrer-Agasson The University of Manchester, Manchester M13 9PL, United Kingdom
N Nayak Brookhaven National Laboratory (BNL), Upton, New York 11973, USA
M Nebot-Guinot University of Edinburgh, Edinburgh EH9 3FD, United Kingdom
J Nowak Lancaster University, Lancaster LA1 4YW, United Kingdom
N Oza Columbia University, New York, New York 10027, USA
O Palamara Fermi National Accelerator Laboratory (FNAL), Batavia, Illinois 60510, USA
N Pallat University of Minnesota, Minneapolis, Minnesota 55455, USA
V Paolone University of Pittsburgh, Pittsburgh, Pennsylvania 15260, USA
A Papadopoulou Argonne National Laboratory (ANL), Lemont, Illinois 60439, USA
V Papavassiliou New Mexico State University (NMSU), Las Cruces, New Mexico 88003, USA
H B Parkinson University of Edinburgh, Edinburgh EH9 3FD, United Kingdom
S F Pate New Mexico State University (NMSU), Las Cruces, New Mexico 88003, USA
N Patel Lancaster University, Lancaster LA1 4YW, United Kingdom
Z Pavlovic Fermi National Accelerator Laboratory (FNAL), Batavia, Illinois 60510, USA
E Piasetzky Tel Aviv University, Tel Aviv, Israel, 69978
I Pophale Lancaster University, Lancaster LA1 4YW, United Kingdom
X Qian Brookhaven National Laboratory (BNL), Upton, New York 11973, USA
J L Raaf Fermi National Accelerator Laboratory (FNAL), Batavia, Illinois 60510, USA
V Radeka Brookhaven National Laboratory (BNL), Upton, New York 11973, USA
A Rafique Argonne National Laboratory (ANL), Lemont, Illinois 60439, USA
M Reggiani-Guzzo University of Edinburgh, Edinburgh EH9 3FD, United Kingdom The University of Manchester, Manchester M13 9PL, United Kingdom
L Ren New Mexico State University (NMSU), Las Cruces, New Mexico 88003, USA
L Rochester SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA
J Rodriguez Rondon South Dakota School of Mines and Technology (SDSMT), Rapid City, South Dakota 57701, USA
M Rosenberg Tufts University, Medford, Massachusetts 02155, USA
M Ross-Lonergan Los Alamos National Laboratory (LANL), Los Alamos, New Mexico 87545, USA
C Rudolf von Rohr Universität Bern, Bern CH-3012, Switzerland
I Safa Columbia University, New York, New York 10027, USA
G Scanavini Wright Laboratory, Department of Physics, Yale University, New Haven, Connecticut 06520, USA
D W Schmitz University of Chicago, Chicago, Illinois 60637, USA
A Schukraft Fermi National Accelerator Laboratory (FNAL), Batavia, Illinois 60510, USA
W Seligman Columbia University, New York, New York 10027, USA
M H Shaevitz Columbia University, New York, New York 10027, USA
R Sharankova Fermi National Accelerator Laboratory (FNAL), Batavia, Illinois 60510, USA
J Shi University of Cambridge, Cambridge CB3 0HE, United Kingdom
E L Snider Fermi National Accelerator Laboratory (FNAL), Batavia, Illinois 60510, USA
M Soderberg Syracuse University, Syracuse, New York 13244, USA
S Söldner-Rembold The University of Manchester, Manchester M13 9PL, United Kingdom
J Spitz University of Michigan, Ann Arbor, Michigan 48109, USA
M Stancari Fermi National Accelerator Laboratory (FNAL), Batavia, Illinois 60510, USA
J St John Fermi National Accelerator Laboratory (FNAL), Batavia, Illinois 60510, USA
T Strauss Fermi National Accelerator Laboratory (FNAL), Batavia, Illinois 60510, USA
A M Szelc University of Edinburgh, Edinburgh EH9 3FD, United Kingdom
W Tang University of Tennessee, Knoxville, Tennessee 37996, USA
N Taniuchi University of Cambridge, Cambridge CB3 0HE, United Kingdom
K Terao SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA
C Thorpe Lancaster University, Lancaster LA1 4YW, United Kingdom The University of Manchester, Manchester M13 9PL, United Kingdom
D Torbunov Brookhaven National Laboratory (BNL), Upton, New York 11973, USA
D Totani University of California, Santa Barbara, California 93106, USA
M Toups Fermi National Accelerator Laboratory (FNAL), Batavia, Illinois 60510, USA
Y-T Tsai SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA
J Tyler Kansas State University (KSU), Manhattan, Kansas 66506, USA
M A Uchida University of Cambridge, Cambridge CB3 0HE, United Kingdom
T Usher SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA
B Viren Brookhaven National Laboratory (BNL), Upton, New York 11973, USA
M Weber Universität Bern, Bern CH-3012, Switzerland
H Wei Louisiana State University, Baton Rouge, Louisiana 70803, USA
A J White University of Chicago, Chicago, Illinois 60637, USA
S Wolbers Fermi National Accelerator Laboratory (FNAL), Batavia, Illinois 60510, USA
T Wongjirad Tufts University, Medford, Massachusetts 02155, USA
M Wospakrik Fermi National Accelerator Laboratory (FNAL), Batavia, Illinois 60510, USA
K Wresilo University of Cambridge, Cambridge CB3 0HE, United Kingdom
W Wu University of Pittsburgh, Pittsburgh, Pennsylvania 15260, USA
E Yandel University of California, Santa Barbara, California 93106, USA
T Yang Fermi National Accelerator Laboratory (FNAL), Batavia, Illinois 60510, USA
L E Yates Fermi National Accelerator Laboratory (FNAL), Batavia, Illinois 60510, USA
H W Yu Brookhaven National Laboratory (BNL), Upton, New York 11973, USA
G P Zeller Fermi National Accelerator Laboratory (FNAL), Batavia, Illinois 60510, USA
J Zennamo Fermi National Accelerator Laboratory (FNAL), Batavia, Illinois 60510, USA
C Zhang Brookhaven National Laboratory (BNL), Upton, New York 11973, USA

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Structure-based, deep-learning models for protein-ligand binding affinity prediction

The launch of AlphaFold series has brought deep-learning techniques into the molecular structural science. As another crucial problem, structure-based prediction of protein-ligand binding affinity urgently calls for advanced computational techniques. Is deep learning ready to decode this problem? Here we review mainstream structure-based, deep-learning approaches for this problem, focusing on molecular representations, learning architectures and model interpretability. A model taxonomy has been generated. To compensate for the lack of valid comparisons among those models, we realized and evaluated representatives from a uniform basis, with the advantages and shortcomings discussed. This review will potentially benefit structure-based drug discovery and related areas.

Comparative proteomic analysis of vancomycin-sensitive and vancomycin-intermediate resistant Staphylococcus aureus

PURPOSE

The extensive use of vancomycin has led to the development of Staphylococcus aureus strains with varying degrees of resistance to vancomycin. The present study aimed to explore the molecular causes of vancomycin resistance by conducting a proteomics analysis of subcellular fractions isolated from vancomycin-intermediate resistant S. aureus (VISA) and vancomycin-sensitive S. aureus (VSSA) strains.

METHODS

We conducted proteomics analysis of subcellular fractions isolated from 2 isogenic S. aureus strains: strain 11 (VSSA) and strain 11Y (VISA). We used an integrated quantitative proteomics approach assisted by bioinformatics analysis, and comprehensively investigated the proteome profile. Intensive bioinformatics analysis, including protein annotation, functional classification, functional enrichment, and functional enrichment-based cluster analysis, was used to annotate quantifiable targets.

RESULTS

We identified 128 upregulated proteins and 21 downregulated proteins in strain 11Y as compared to strain 11. The largest group of differentially expressed proteins was composed of enzymatic proteins associated with metabolic and catalytic activity, which accounted for 32.1% and 50% of the total proteins, respectively. Some proteins were indispensable parts of the regulatory networks of S. aureus that were altered with vancomycin treatment, and these proteins were related to cell wall metabolism, cell adhesion, proteolysis, and pressure response.

CONCLUSION

Our proteomics study revealed regulatory proteins associated with vancomycin resistance in S. aureus. Some of these proteins were involved in the regulation of cell metabolism and function, which provides potential targets for the development of strategies to manage vancomycin resistance in S. aureus.

Dietary inflammatory index is associated with Vitamin D in CKD patients

OBJECTIVES

Multiple observational studies have shown that low serum level of 25-hydroxyvitamin D (25(OH)D) in patients with chronic kidney disease (CKD) have been associated with a faster progression of kidney disease and a higher risk of all-cause mortality. We aim to assess the association between dietary inflammatory index (DII) with Vitamin D in adults with CKD.

METHOD

The National Health and Nutrition Examination Survey appropriated participants from 2009 to 2018 were enrolled. The patients who were under the age of 18, pregnant, and having incomplete data were excluded. DII score were calculated based on a single 24-h dietary recall interview for each participant. Mutivariable regression analysis and subgroup analysis were utilized to determine the independent associations between vitamin D with DII in CKD patients.

RESULTS

In total, 4283 individuals were finally included. The results showed a negative association between DII scores and 25(OH)D with statistical significance (β =  - 1.83, 95% CI  - 2.31,  - 1.34, P < 0.001). In subgroup analysis stratified by gender, low eGFR, age and diabetes, the negative association between DII scores and 25(OH)D was still significant (all P for trend < 0.05). The results from interacion test indicated that the magnitude of the association was the same for the population with and without low eGFR (P for interacion = 0.464).

CONCLUSION

Higher consumption of pro-inflammatory diet correlates negatively with the 25(OH)D level in CKD patients with and without low eGFR. Anti-inflammatory diet management may reduce the reduction of vitamin D in CKD patients.

The effects of adenoid hypertrophy and oral breathing on maxillofacial development: a review of the literature

According to modern epidemiological surveys, the prevalence of adenoid hypertrophy in children and adolescents ranges from 42% to 70%. Adenoid hypertrophy can lead to airway obstruction; thus forces a child to breathe through their mouth, thus affecting the normal development of the dental and maxillofacial area, and can lead to malocclusion. Long-term mouth breathing can cause sagittal, vertical and lateral changes in the maxillofacial area. In this article, we review the current research status relating to the association between adenoid hypertrophy, oral breathing and maxillofacial growth and development in children and adolescents. We also discuss the personalized formulation of treatment plans.

Isothermal Amplification and CRISPR/Cas12a-System-Based Assay for Rapid, Sensitive and Visual Detection of Staphylococcus aureus

Staphylococcus aureus exists widely in the natural environment and is one of the main food-borne pathogenic microorganisms causing human bacteremia. For safe food management, a rapid, high-specificity, sensitive method for the detection of S. aureus should be developed. In this study, a platform for detecting S. aureus (nuc gene) based on isothermal amplification (loop-mediated isothermal amplification-LAMP, recombinase polymerase amplification-RPA) and the clustered regularly interspaced short palindromic repeats (CRISPR) and CRISPR-associated (Cas12a) proteins system (LAMP, RPA-CRISPR/Cas12a) was proposed. In this study, the LAMP, RPA-CRISPR/Cas12a detection platform and immunochromatographic test strip (ICS) were combined to achieve a low-cost, simple and visualized detection of S. aureus. The limit of visual detection was 57.8 fg/µL of nuc DNA and 6.7 × 102 CFU/mL of bacteria. Moreover, the platform could be combined with fluorescence detection, namely LAMP, RPA-CRISPR/Cas12a-flu, to establish a rapid and highly sensitive method for the detection of S. aureus. The limit of fluorescence detection was 5.78 fg/µL of genomic DNA and 67 CFU/mL of S. aureus. In addition, this detection platform can detect S. aureus in dairy products, and the detection time was ~40 min. Consequently, the isothermal amplification CRISPR/Cas12a platform is a useful tool for the rapid and sensitive detection of S. aureus in food.

Comparisons between young adult waterpipe smokers and nonsmokers' reactions to pictorial health warning labels in Lebanon: a randomized crossover experimental study

This study compares the impact of pictorial health warning labels (HWLs) and their placements on waterpipe parts (device, tobacco and charcoal packages) on health communication outcomes between waterpipe smokers and nonsmokers in Lebanon. An online randomized crossover experimental study was conducted among young adults (n = 403, August 2021) who observed three conditions of HWLs: pictorial HWLs on the tobacco package, pictorial HWLs on all waterpipe's parts and text-only HWL on the tobacco package in random order. Participants completed post-exposure assessments of health communication outcomes after each image. Using linear mixed models, we examined the differences in the effect of HWL conditions on several outcomes (i.e. warning reactions) between waterpipe smokers and nonsmokers, controlling for confounders (i.e. age, sex). Nonsmokers reported greater attention (β = 0.54 [95% confidence interval: 0.25-0.82]), cognitive elaboration (0.31 [0.05-0.58]) and social interaction (0.41 [0.18-0.65]) for pictorial HWLs on the tobacco packages than text-only compared with smokers. Pictorial HWLs on three parts versus one part elicited higher cognitive reactions and perceived message effectiveness in nonsmokers compared with waterpipe smokers. These findings provide valuable information for policymakers about the potential of implementing HWLs specific to waterpipes to prevent their use among young adults and limit tobacco-related morbidity and mortality in Lebanon.

Targeting the E2F1/Rb/HDAC1 axis with the small molecule HR488B effectively inhibits colorectal cancer growth

Colorectal cancer (CRC), the third most common cancer worldwide, remains highly lethal as the disease only becomes symptomatic at an advanced stage. Growing evidence suggests that histone deacetylases (HDACs), a group of epigenetic enzymes overexpressed in precancerous lesions of CRC, may represent promising molecular targets for CRC treatment. Histone deacetylase inhibitors (HDACis) have gradually become powerful anti-cancer agents targeting epigenetic modulation and have been widely used in the clinical treatment of hematologic malignancies, while only few studies on the benefit of HDACis in the treatment of CRC. In the present study, we designed a series of small-molecule Thiazole-based HDACis, among which HR488B bound to HDAC1 with a high affinity and exerted effective anti-CRC activity both in vitro and in vivo. Moreover, we revealed that HR488B specifically suppressed the growth of CRC cells by inducing cell cycle G0/G1 arrest and apoptosis via causing mitochondrial dysfunction, reactive oxygen species (ROS) generation, and DNA damage accumulation. Importantly, we noticed that HR488B significantly decreased the expression of the E2F transcription factor 1 (E2F1), which was crucial for the inhibitory effect of HR488B on CRC. Mechanistically, HR488B obviously decreased the phosphorylation level of the retinoblastoma protein (Rb), and subsequently prevented the release of E2F1 from the E2F1/Rb/HDAC1 complex, which ultimately suppressed the growth of CRC cells. Overall, our study suggests that HR488B, a novel and efficient HDAC1 inhibitor, may be a potential candidate for CRC therapy in the future. Furthermore, targeting the E2F1/Rb/HDAC1 axis with HR488B provides a promising therapeutic avenue for CRC.

MiR-122-5p as a potential regulator of pulmonary vascular wall cell in idiopathic pulmonary arterial hypertension

MicroRNAs (miRNAs) are versatile regulators of pulmonary arterial remodeling in idiopathic pulmonary arterial hypertension (IPAH). We herein aimed to characterize miRNAs in peripheral blood mononuclear cell (PBMC) and plasma exosomes, and investigate specific miRNA expression in pulmonary artery cells and lung tissues in IPAH. A co-dysregulated miRNA was identified from the miRNA expression profiles of PBMC and plasma exosomes in IPAH. Gene Ontology (GO) and Kyoto Encyclopedia of Genes and Genomes (KEGG) analysis revealed the potential function of differentially expressed miRNAs. Real-time quantitative reverse transcription polymerase chain reaction was used to validate the expression of specific miRNAs in hypoxia-induced pulmonary microvascular endothelial cells (PMECs), pulmonary artery smooth muscle cells (PASMCs), pericyte cells (PCs), and lung tissues of patients with IPAH and rats. Finally, the miRNA-mRNA mechanisms of miR-122-5p were predicted. MiR-122-5p was the only co-upregulated miRNA in PBMC and plasma exosomes in patients with IPAH. Functional analysis of differentially expressed miRNAs revealed associations with the GO terms "transcription, DNA-templated," "cytoplasm," and "metal ion binding" in both PBMC and plasma exosomes, KEGG pathway MAPK signaling in PBMC, and KEGG-pathway human papillomavirus infection in plasma exosomes. Hypoxic PMECs and PCs, lung tissue of patients with IPAH, and rats showed increased expression of miR-122-5p, but hypoxic PASMCs showed decreased expression. And miR-122-5p mimics and inhibitor affected cell proliferation. Finally, miR-122-5p was found to potentially target DLAT (in lung tissue) and RIMS1 (in PMECs) in IPAH. According to the dual-luciferase assay, miR-122-5p bound to DLAT or RIMS1. In studies, DLAT imbalance was associated with cell proliferation and migration, RIMS1 is differentially expressed in cancer and correlated with cancer prognosis. Our findings suggest that the miR-122-5p is involved in various biological functions in the adjacent vascular wall cells in IPAH.

Construction of an EMT-related lncRNA prognostic signature for lung adenocarcinoma and functional verification of its hub gene LINC01615

BACKGROUND

The epithelial-mesenchymal transition (EMT) plays a vital role in the progression of lung adenocarcinoma (LUAD). Long non-coding RNAs (lncRNAs) participate in the EMT process as an important regulatory factor and have the potential to serve as prognostic biomarkers. We aimed to construct a novel lncRNA prognostic signature for LUAD based on EMT-related lncRNAs, identify EMT-related hub lncRNA, and investigate its biological functions.

METHODS

RNA-seq data, clinical and survival information were obtained from The Cancer Genome Atlas database. The EMT-related lncRNA prognostic signature (EMTscore) was constructed using the Least Absolute Shrinkage and Selection Operator Cox regression analysis. The efficiency of EMTscore in predicting the prognosis of LUAD was evaluated through the area under the time-dependent receiver operating characteristic (ROC) curves. The hub lncRNA of the prognostic signature was selected using a co-expression network map, and its effects on cell proliferation and metastasis were explored by in vitro experiments.

RESULTS

We constructed a prognostic signature (EMTscore) containing 8 tumor-high expressed lncRNAs. The EMTscore performed well in predicting overall survival rates with AUC values of 0.708 at 5 years in the training set. EMTscore could independently predict the survival of LUAD, with HR = 4.011 (95% CI 2.430-6.622) in the multivariate Cox regression. Importantly, we identified LINC01615 as the hub lncRNA in the EMTscore and revealed that LINC01615 enhanced the proliferation, migration, and EMT of lung cancer cells.

CONCLUSIONS

A new EMT-related lncRNA prognostic signature named EMTscore was developed, and LINC01615 was identified as the hub lncRNA of EMTscore. The hub lncRNA LINC01615 had an oncogenic biological function in LUAD.

Transanal local excision for mucosal prolapse syndrome

A 46-year-old male visited our hospital with blood stool and constipation. Colonoscopy revealed a broad-based protruded lesion in the rectum.The endoscopic ultrasonography showed the lesion invaded the submucosa, and the boundary between the local and intrinsic muscular layer was not clear. Transanal local excision was conducted, the pathology showed a rare case of mucosal prolapse syndrome merging chronic suppurative inflammation.

[Clinical characteristics analysis of patients with severe immune checkpoint inhibitors related myocarditis]

Objective: To analyze the clinical characteristics of patients with severe immune checkpoint inhibitors (ICIs) related myocarditis. Methods: A retrospective study was conducted on the 50 patients with ICIs-related myocarditis in the multidisciplinary cardio-oncology clinic of Zhongshan Hospital affiliated to Fudan University from April 2020 to April 2022. The age of patients was (63.7±10.8) years old, including 37 males and 13 females. The patients were divided into the mild group (n=37) and the severe group (n=13) according to severity. The differences of basic characteristics, clinical manifestations, laboratory tests, auxiliary examination, combined irAEs, treatment and outcomes between the two groups of patients were analyzed. Results: The immunotherapy time [M(Q1,Q3)] of patients in the mild group and severe group were 81 (49, 134) and 24 (20, 116) days, respectively (P<0.05). In the severe group, the levels of cTnT [0.605 (0.317, 1.072) μg/L], NT-proBNP [1 126 (386, 1 744) ng/L], CK-MB [78 (48, 238) U/L], and CK-MM [240 (45, 6 543) U/L] were higher than those in the mild group [0.104 (0.045, 0.189) μg/L, 237 (39, 785) ng/L, 24 (20, 33) U/L, 108 (72, 168) U/L, respectively] (all P<0.05). The left ventricular ejection fraction of the severe group [64% (57%, 65%)] was lower than that of the mild group [66% (63%, 69%)] (P<0.05), and the incidence of conduction block (n=4, 4/13) and abnormal ventricular wall motion (n=4, 4/13), the incidence of ICIs-related myositis (n=10, 10/13), ICIs-related hepatitis (n=4, 4/13) and ICIs-related neurotoxicity (n=4, 4/13) were higher than those in the mild group (n=1, 2.7%; n=2, 5.4%; n=16, 43.2%; n=2, 5.4%; n=1, 2.7%, respectively) (all P<0.05). The proportion of patients receiving intensified immunosuppressive therapy and mortality rate in the severe group were 12/13 (n=12) and 4/13 (n=4), which were both higher than those in the mild group [10.8% (n=4) and 0] (both P<0.05). Conclusions: The incidence of ICIs-related myocarditis is not high, but the severe rate and mortality are high. The differential diagnosis of severe ICIs related myocarditis should be combined with myocardial markers, electrocardiogram and echocardiogram, and early diagnosis and treatment can improve the prognosis of patients.

[Clinical and molecular biological characterization of patients with accelerated chronic lymphocytic leukemia]

Objective: To investigate the clinical and molecular biological characteristics of patients with accelerated chronic lymphocytic leukemia (aCLL) . Methods: From January 2020 to October 2022, the data of 13 patients diagnosed with aCLL at The First Affiliated Hospital of Nanjing Medical University were retrospectively analyzed to explore the clinical and molecular biological characteristics of aCLL. Results: The median age of the patients was 54 (35-72) years. Prior to aCLL, five patients received no treatment for CLL/small lymphocytic lymphoma (SLL), while the other patients received treatment, predominantly with BTK inhibitors. The patients were diagnosed with aCLL through pathological confirmation upon disease progression. Six patients exhibited bulky disease (lesions with a maximum diameter ≥5 cm). Positron emission tomography (PET) -computed tomography (CT) images revealed metabolic heterogeneity, both between and within lesions, and the median maximum standardized uptake value (SUVmax) of the lesion with the most elevated metabolic activity was 6.96 (2.51-11.90). Patients with unmutated IGHV CLL accounted for 76.9% (10/13), and the most frequent genetic and molecular aberrations included +12 [3/7 (42.9% ) ], ATM mutation [6/12 (50% ) ], and NOTCH1 mutation [6/12 (50% ) ]. Twelve patients received subsequent treatment. The overall response rate was 91.7%, and the complete response rate was 58.3%. Five patients experienced disease progression, among which two patients developed Richter transformation. Patients with aCLL with KRAS mutation had worse progression-free survival (7.0 month vs 26.3 months, P=0.015) . Conclusion: Patients with aCLL exhibited a clinically aggressive course, often accompanied by unfavorable prognostic factors, including unmutated IGHV, +12, ATM mutation, and NOTCH1 mutation. Patients with CLL/SLL with clinical suspicion of disease progression, especially those with bulky disease and PET-CT SUVmax ≥5, should undergo biopsy at the site of highest metabolic uptake to establish a definitive pathological diagnosis.

Measurements of Groomed-Jet Substructure of Charm Jets Tagged by D^{0} Mesons in Proton-Proton Collisions at sqrt[s]=13 TeV

Understanding the role of parton mass and Casimir color factors in the quantum chromodynamics parton shower represents an important step in characterizing the emission properties of heavy quarks. Recent experimental advances in jet substructure techniques have provided the opportunity to isolate and characterize gluon emissions from heavy quarks. In this Letter, the first direct experimental constraint on the charm-quark splitting function is presented, obtained via the measurement of the groomed shared momentum fraction of the first splitting in charm jets, tagged by a reconstructed D^{0} meson. The measurement is made in proton-proton collisions at sqrt[s]=13  TeV, in the low jet transverse-momentum interval of 15≤p_{T}^{jet ch}<30  GeV/c where the emission properties are sensitive to parton mass effects. In addition, the opening angle of the first perturbative emission of the charm quark, as well as the number of perturbative emissions it undergoes, is reported. Comparisons to measurements of an inclusive-jet sample show a steeper splitting function for charm quarks compared with gluons and light quarks. Charm quarks also undergo fewer perturbative emissions in the parton shower, with a reduced probability of large-angle emissions.

Impact of reduced apolipoprotein A-I levels on pulmonary arterial hypertension

BACKGROUND

The significance of apolipoprotein A-I (ApoA-I) is the anti-inflammatory functional component of high-density lipoprotein, which needs to be further studied in relation to pulmonary arterial hypertension (PAH). This study aimed to identify the predictive value of ApoA-1 on the risk and prognosis of PAH, as well as the underlying anti-inflammatory mechanism.

METHODS

Proteomic analysis was conducted on lung tissue from 6 PAH patients and 4 lung donors. Prediction of risk and mortality risk factors associated with PAH in 343 patients used logistic analysis and Cox regression analysis, respectively. The protective function of ApoA-I was assessed in human pulmonary arterial endothelial cells (HPAEC), while its anti-inflammatory function was evaluated in THP-1 macrophages.

RESULTS

In the lung tissues of patients with PAH, 168 differentially expressed proteins were associated with lipid metabolism according to GO and KEGG enrichment analysis. A protein-protein interaction network identified ApoA-I as a key protein associated with PAH. Lower ApoA-I levels were independent risk factors for PAH and displayed a stronger predictive value for PAH mortality. Plasma interleukin 6 (IL-6) levels were positively correlated with risk stratification and was higher in PAH patients with lower ApoA-I levels. ApoA-I was downregulated in lung tissues of MCT-induced rats. ApoA-I could reduce IL-6-induced pro-proliferative and pro-migratory abilities of HPAEC and inhibit secretion of IL-6 from macrophages, which is compromised under hypoxic conditions.

CONCLUSION

Our study identified the significance of ApoA-I as a biomarker for predicting the survival outcome of PAH patients, which might relate to its altered anti-inflammatory properties.

Validation of a shortened MR imaging protocol for pediatric spinal pathology

OBJECTIVE

Conventional pediatric spine MRI protocols have multiple sequences resulting in long acquisition times. Sedation is consequently required. This study evaluates the diagnostic capability of a limited MRI spine protocol for selected common pediatric indications.

METHODS

Spine MRIs at CHEO between 2017 and 2020 were reviewed across pediatric patients younger than four years old. Two blinded neuroradiologists reviewed limited scan sequences, and results were independently compared to previously reported findings from the complete imaging series. T2 sagittal sequences from the craniocervical junction to sacrum and T1 axial sequence of the lumbar spine constitute the short protocol, with the outcomes of interest being cerebellar ectopia, syrinx, level of conus, filum < 2 mm, fatty filum, and spinal dysraphism.

RESULTS

A total of 105 studies were evaluated in 54 male and 51 female patients (mean age 19.2 months). The average combined scan time of the limited sequences was 15 min compared to 35 min for conventional protocols (delta = 20 min). The average percent agreement between full and limited sequences was > 95% in all but identifying a filum < 2 mm, where the percent agreement was 87%. Using limited MR sequences had high sensitivity (> 0.91) and specificity (> 0.99) for the detection of cerebellar ectopia, syrinx, fatty filum, and spinal dysraphism.

CONCLUSION

This study demonstrates that selected spinal imaging sequences allow for consistent and accurate diagnosis of specific clinical conditions. A limited spine imaging protocol has potential as a screening test to reduce the need for full-sequence MRI scans. Further work is needed to determine utility of selected imaging for other clinical indications.

Dose Painting Radiotherapy Guided by Diffusion-Weighted Magnetic Resonance vs. 18F-FDG-PET/CT in Locoregionally Advanced Nasopharyngeal Carcinoma: A Randomized, Controlled Clinical Trial

PURPOSE/OBJECTIVE(S)

This phase II randomized controlled trial aimed at comparing the efficacy and toxicity of diffusion-weighted magnetic resonance imaging (DWI)-guided dose painting radiotherapy (DP-RT), FDG-PET/CT-guided DP-RT, and conventional MRI-based radiotherapy (RT) in locoregionally advanced nasopharyngeal carcinoma (NPC).

MATERIALS/METHODS

A total of 330 patients with stage III-IVa NPC disease were randomly assigned in a 1:1:1 ratio to receive induction chemotherapy followed by concurrent chemoradiotherapy by DWI-guided DP-RT (group A, n = 110), FDG-PET/CT-guided DP-RT (group B, n = 110), or conventional MRI-based RT (group C, n = 110). All patients received volumetric modulated arc therapy (VMAT). In group A, subvolume GTVnx-DWI (gross tumor volume of nasopharynx in DWI) was defined as the areas within the GTVnx (gross tumor volume of nasopharynx) with an apparent diffusion coefficient (ADC) below the mean ADC (ADC < mean). In group B, subvolume GTVnx-PET (gross tumor volume of nasopharynx in PET images) was defined within GTVnx as the SUV50%max isocontour. The doses to GTVnx-DWI in group A and GTVnx-PET in group B were escalated to 75.2 Gy/32 fx in patients with T1-2 disease and to 77.55 Gy/33 fx in those with T3-4 disease in 2.35 Gy per fraction. In group C, planning gross tumor volume of nasopharynx (PGTVnx) was irradiated at 70.4 to 72.6 Gy/32 to 33 fx in 2.2 Gy per fraction. This trial is registered with chictr.org.cn (ChiCTR2200057476).

RESULTS

Group A and B showed significant higher complete response (CR) rates than group C (100%, 100%, and 96.4% for group A, B and C, respectively, p = 0.036). In groups A, B and C, the 1-year local recurrence-free survival (LRFS) rates were 100%, 100%, and 94.5%, respectively (p = 0.002). The 1-year disease-free survival (DFS) rates were 100%, 99.1%, and 92.7%, respectively (p = 0.001). The 1-year distant metastasis-free survival (DMFS) rates were 100%, 99.1%, and 93.6%, respectively (p = 0.004). The 1-year overall survival (OS) rates were 100%, 100%, and 95.4%, respectively (p = 0.006). Group A and B had significantly higher 1-year LRFS, DFS, DMFS, and OS than those in group C. No significant differences were observed in LRFS, DFS, DMFS and OS between group A and B. Group B (PET/CT group) had a higher incidence of grade 3-4 acute ototoxicity (3.6%) than group A (0%) and group C (0%, p = 0.036). No significant differences in other grade 3-4 acute adverse events and late toxic effects were observed among the three groups, and no patient had grade 5 toxicities. Multivariate analysis showed that dose painting (DWI-guided DP-RT and PET/CT-guided DP-RT vs conventional MRI-based RT) was associated with improved LRFS, DFS, DMFS and OS.

CONCLUSION

Both DWI-guided DP-RT and PET/CT-guided DP-RT plus chemotherapy are associated with improved LRFS, DFS, DMFS and OS compared with conventional MRI-based RT among patients with locoregionally advanced NPC. DWI-guided DP-RT does not increase toxicities, but PET/CT-guided DP-RT has higher incidence of acute ototoxicity.

Safe and Durable Treatment of Dentin Hypersensitivity via Nourishing and Remineralizing Dentin Based on β-Chitooligosaccharide Graft Derivative

Dentin hypersensitivity (DH) is a common symptom of various dental diseases that usually produces abnormal pain with external stimuli. Various desensitizers are developed to treat DH by occluding dentine tubules (DTs) or blocking intersynaptic connections of dental sensory nerve cells. However, the main limitations of currently available techniques are the chronic toxic effects of chemically active ingredients and their insufficiently durable efficacy. Herein, a novel DH therapy with remarkable biosafety and durable therapeutic value based on β-chitooligosaccharide graft derivative (CAD) is presented. Particularly, CAD indicates the most energetic results, restoring the amino polysaccharide protective membrane in DTs, significantly promoting calcium and phosphorus ion deposition and bone anabolism, and regulating the levels of immunoglobulin in saliva and cellular inflammatory factors in plasma. Exposed DTs are occluded by remineralized hydroxyapatite with a depth of over 70 µm, as shown in in vitro tests. The bone mineral density of Sprague-Dawley rats' molar dentin increases by 10.96%, and the trabecular thickness of bone improves to about 0.03 µm in 2 weeks in the CAD group compared to the blank group. Overall, the ingenious concept that modified marine biomaterial can be a safe and durable therapy for DH is demonstrated by nourishing and remineralizing dentin.

Efficacy and Toxicity of Different Target Volume Delineations of Radiotherapy Based on the Updated RTOG/NRG and EORTC Guidelines in Patients with High Grade Glioma: A Randomized, Controlled Clinical Trial

PURPOSE/OBJECTIVE(S)

Postoperative radiotherapy with concomitant and adjuvant temozolomide (TMZ) is the standard of care for newly diagnosed high grade glioma, but the optimal method for target volume delineations for intensity modulated radiation therapy (IMRT) is still unclear. We hypothesized that compared with the EORTC guidelines, IMRT based on the updated RTOG/NRG guidelines was equally effective, without increasing toxicities for patients with high-grade glioma. The purpose of this randomized phase 2 study was to compare the efficacy and toxicity of IMRT based on different target volume delineations (updated RTOG/NRG versus EORTC guidelines) with concomitant and adjuvant TMZ for patients with high grade glioma.

MATERIALS/METHODS

A total of 302 patients with newly diagnosed high-grade glioma (WHO grade 3-4) were randomly assigned (1:1) to receive postoperative IMRT based on either updated RTOG/NRG guidelines (RTOG/NRG group, n = 151) or EORTC guideline (EORTC group, n = 151), with concomitant and adjuvant TMZ. In the RTOG/NRG group, an initial volume consisting of enhancement, postoperative cavity, plus surrounding edema (or fluid-attenuated inversion recovery [FLAIR] abnormality defined by magnetic resonance imaging [MRI]) and a 2-cm margin received 46 Gy in 23 fractions followed by a boost of 14 Gy in 7 fractions to the area of enhancement plus the cavity and a 2-cm margin. In the EORTC group, a single planning volume was used to deliver 60 Gy in 30 fractions to the area of enhancement and the cavity with a 2-cm margin. The primary end point was overall survival (OS). Secondary end points included progression-free survival (PFS) and toxicities associated with each treatment.

RESULTS

No statistically significant differences were observed between groups for 1-year OS (71.8% for RTOG/NRG group and 69.9% for EORTC group, respectively; P = 0.759) or 1-year PFS (46.7% for RTOG/NRG group and 43.6% for EORTC group, respectively; P = 0.674). Efficacy did not differ by MGMT methylation status. There were no differences in grade 3-4 toxicities (leukopenia, lymphopenia, neutropenia, thrombocytopenia, fatigue, nausea and vomiting) between the two groups. No grade 5 toxicities were observed in both groups. Multivariate analyses showed that tumor MGMT status (methylated vs unmethylated) and WHO grade (grade 3 vs grade 4) were associated with OS and PFS. However, radiation type (RTOG/NRG group vs EORTC), sex, age, and Karnofsky scale did not significantly influence OS or PFS.

CONCLUSION

Compared with EORTC guidelines for postoperative radiotherapy, IMRT based on RTOG/NRG guidelines was equally effective, without increasing toxicities for patients with high-grade glioma. This trial is registered with chictr.org.cn, number ChiCTR2100046667.

A Pilot Study of Stereotactic Body Radiotherapy and 177Lu-PSMA-617 for Oligometastatic Hormone Sensitive Prostate Cancer

PURPOSE/OBJECTIVE(S)

Stereotactic body radiotherapy (SBRT) is increasingly used for oligorecurrent prostate cancer (OPC). Despite excellent local control, distant metastasis free survival rates are more modest. We hypothesized SBRT outcomes could be optimized with improved staging imaging and integration of a well-tolerated targeted radiopharmaceutical therapy (RLT) for microscopic disease. We report initial results of a prospective, single-institution pilot (NCT05079698) of a novel, PSMA-based theranostic strategy for OPC.

MATERIALS/METHODS

Men with castrate sensitive OPC and 1-3 sites of PSMA PET avid disease ("index lesions") and no PSMA non-avid sites were eligible. No androgen deprivation therapy was permitted. Subjects first received 2 cycles of 177Lu-PSMA-617 RLT (7.47±0.14 GBq) spaced 6 weeks apart. In vivo dosimetry was performed during cycle 1. Four weeks post-cycle 2, patients were restaged with 68Ga-PSMA PET for an interim (post-RLT) response assessment. Index lesions were then consolidated with SBRT (9 Gy x 3) irrespective of post-RLT PET response. The primary outcome was feasibility defined as successful completion of protocol-mandated therapy without intercurrent distant failure on post-RLT PET.

RESULTS

Six men were treated with nine total index lesions (5 nodal, 3 osseous, 1 visceral). The study met its primary endpoint; all completed required interventions and no distant progression was seen on interim PSMA PET. Treatment was well tolerated; no grade 3+ toxicities, 2/6 had grade 2 toxicities (transient anemia and hyperbilirubinemia) and 5/6 had grade 1 toxicities. Median baseline lesion-level PSMA SUVmax was 16.8±8.7. Median interim SUVmax was 6.2±2.5 and declined for all but one lesion post-RLT (median -65%). Median SUVmax at 3-mos post-SBRT was 3.3±2.5 and decreased for all evaluable lesions (median -80%). Median baseline PSA was 2.01 ng/mL (range: 0.72-4.56) which declined in 5/6 post-RLT. The 6th patient experienced biochemical rise with interim PET showing only greater avidity in the known index lesion and SBRT was completed per protocol. All 4 evaluable patients with at least one post-SBRT follow-up have improved PSA at last visit (range 5.5-12 mos from cycle 1), and 2/4 have undetectable PSA. Composite dosimetry, correlatives and quality of life studies are forthcoming.

CONCLUSION

Our pilot study demonstrates the feasibility of a novel PSMA anchored theranostic strategy combining SBRT with targeted RLT for OPC. Preliminary data suggests promising outcomes, including the possibility of achieving an undetectable biochemical disease state without hormone therapy.

[Prognostic significance and immune cell infiltration analysis of differentially expressed genes in malignant pleural mesothelioma]

Objective: To explore and analyze differential expressed genes in malignant pleural mesothelioma (MPM) by bioinformatics method, and to study their prognostic value in MPM and their potential role in immunotherapy. Methods: In January 2022, the dataset GSE51024 was downloaded from the GEO database, and MPM (55 cases) and normal tissue (41 cases) samples were obtained. Using R software and HMDD and miRNet database, MPM-related differential genes were screened and co-expressed genes were identified. Co-expressed genes were enriched and functionally annotated, and protein-protein interaction (PPI) networks were constructed and key genes were identified using the STRING database and Cytoscape software. TRRUST and GEPIA databases were used to predict transcription factors of key genes and to analyze prognosis and survival. The correlation between key genes and the degree of infiltration of immune cells was analyzed using TIMER. Results: A total of 435 co-expressed genes were obtained, which were mainly concentrated in the extracellular matrix tissue and the signaling pathways of cell adhesion molecules. Combined with PPI and TRRUST database, seven key MPM prognostic genes were identified. Among them, cyclin 20 (CDC20) , cell cycle checkpoint kinase 1 (CHEK1) , enhancer of Zeste homolog 2 (EZH2) , ribonucleotide reductase subunit M2 (RRM2) , topoisomerase 2A (TOP2A) , ubiquitin like plant homeodomain and ring finger domain 1 (UHRF1) were significantly up-regulated in MPM, while cyclin A1 (CCNA1) was significantly down-regulated. The expressions of CCNA1, CDC20, CHEK1, EZH2, RRM2, TOP2A and UHRF1 genes were significantly associated with MPM overall survival (P<0.05) . The expressions of CDC20, CHEK1, EZH2, RRM2 and TOP2A genes were positively correlated with B cells and dendritic cells (P<0.05) , and negatively correlated with neutrophils (P<0.05) . Conclusion: CCNA1, CDC20, CHEK1, EZH2, RRM2, TOP2A and UHRF1 may be potential prognostic markers in MPM patients, and their expressions may be related to MPM tumor immunity.

The Impact of Abnormal Lipid Metabolism on the Occurrence Risk of Idiopathic Pulmonary Arterial Hypertension

The aim was to determine whether lipid molecules can be used as potential biomarkers for idiopathic pulmonary arterial hypertension (IPAH), providing important reference value for early diagnosis and treatment. Liquid chromatography-mass spectrometry-based lipidomic assays allow for the simultaneous detection of a large number of lipids. In this study, lipid profiling was performed on plasma samples from 69 IPAH patients and 30 healthy controls to compare the levels of lipid molecules in the 2 groups of patients, and Cox regression analysis was used to identify meaningful metrics, along with receiver operator characteristic curves to assess the ability of the lipid molecules to predict the risk of disease in patients. Among the 14 lipid subclasses tested, 12 lipid levels were significantly higher in IPAH patients than in healthy controls. Free fatty acids (FFA) and monoacylglycerol (MAG) were significantly different between IPAH patients and healthy controls. Logistic regression analysis showed that FFA (OR: 1.239, 95%CI: 1.101, 1.394, p < 0.0001) and MAG (OR: 3.711, 95%CI: 2.214, 6.221, p < 0.001) were independent predictors of IPAH development. Among the lipid subclasses, FFA and MAG have potential as biomarkers for predicting the pathogenesis of IPAH, which may improve the early diagnosis of IPAH.

Fungi Fibrinolytic Compound 1 Plays a Core Role in Modulating Fibrinolysis, Altering Plasma Clot Structure, and Promoting Susceptibility to Lysis

Fibrin clot structure and function are major determinants of venous and arterial thromboembolic diseases, as well as the key determinants of the efficiency of clot lysis. Studies have revealed that fungi fibrinolytic compound 1 (FGFC1) is a novel marine pyranisoindolone natural product with fibrinolytic activity. Here, we explore the impacts of FGFC1 on clot structure, lysis, and plasminogen activation in vitro using turbidimetric, enzyme-linked immunosorbent assay, confocal and electron microscopy, urokinase, or plasmin chromogenic substrate. Clots formed in the presence of FGFC1 expressed reduced fibrin polymerization rate and maximum turbidity; however, they did not influence the lag phase of fibrin polymerization. In the absence of scu-PA (single-chain urokinase plasminogen activator), microscopy revealed that FGFC1 increased the number of protofibrils within fibrin fiber and the pore diameter between protofibrils, inducing clots to form a region of thinner and looser networks separated by large pores. The effects of FGFC1 on scu-PA-mediated plasma clot structure were similar to those in the absence of scu-PA. In addition, FGFC1 promoted the lysis of clots and increased the D-dimer concentration in lysate. FGFC1 increased the generation rate of p-nitroaniline in plasma. These results show that FGFC1 has fibrinolytic activity in plasma, leading to interference with the release of fibrinopeptide B to affect lateral aggregation of protofibrils and increase clot susceptibility to fibrinolysis by altering its structure.

First Double-Differential Measurement of Kinematic Imbalance in Neutrino Interactions with the MicroBooNE Detector

We report the first measurement of flux-integrated double-differential quasielasticlike neutrino-argon cross sections, which have been made using the Booster Neutrino Beam and the MicroBooNE detector at Fermi National Accelerator Laboratory. The data are presented as a function of kinematic imbalance variables which are sensitive to nuclear ground-state distributions and hadronic reinteraction processes. We find that the measured cross sections in different phase-space regions are sensitive to different nuclear effects. Therefore, they enable the impact of specific nuclear effects on the neutrino-nucleus interaction to be isolated more completely than was possible using previous single-differential cross section measurements. Our results provide precision data to help test and improve neutrino-nucleus interaction models. They further support ongoing neutrino-oscillation studies by establishing phase-space regions where precise reaction modeling has already been achieved.

Measurement of the Lifetime and Λ Separation Energy of _{Λ}^{3}H

The most precise measurements to date of the _{Λ}^{3}H lifetime τ and Λ separation energy B_{Λ} are obtained using the data sample of Pb-Pb collisions at sqrt[s_{NN}]=5.02  TeV collected by ALICE at the LHC. The _{Λ}^{3}H is reconstructed via its charged two-body mesonic decay channel (_{Λ}^{3}H→^{3}He+π^{-} and the charge-conjugate process). The measured values τ=[253±11(stat)±6(syst)]  ps and B_{Λ}=[102±63(stat)±67(syst)]  keV are compatible with predictions from effective field theories and confirm that the _{Λ}^{3}H structure is consistent with a weakly bound system.

Dihydroartemisinin attenuates ischemia/reperfusion-induced renal tubular senescence by activating autophagy

Acute kidney injury (AKI) is an important factor for the occurrence and development of CKD. The protective effect of dihydroartemisinin on AKI and and reported mechanism have not been reported. In this study, we used two animal models including ischemia-reperfusion and UUO, as well as a high-glucose-stimulated HK-2 cell model, to evaluate the protective effect of dihydroartemisinin on premature senescence of renal tubular epithelial cells in vitro and in vivo. We demonstrated that dihydroartemisinin improved renal aging and renal injury by activating autophagy. In addition, we found that co-treatment with chloroquine, an autophagy inhibitor, abolished the anti-renal aging effect of dihydroartemisinin in vitro. These findings suggested that activation of autophagy/elimination of senescent cell might be a useful strategy to prevent AKI/UUO induced renal tubular senescence and fibrosis.

LincRNA-EPS Alleviates Inflammation in TMJ Osteoarthritis by Binding to SRSF3

Temporomandibular joint osteoarthritis (TMJOA) is a common inflammatory disease that can cause pain, cartilage degradation, and subchondral bone loss. However, the key regulatory factors and new targets for the treatment of TMJOA have yet to be determined. Long noncoding RNAs (lncRNAs) have shown remarkable potential in regulating tissue homeostasis and disease development. The long intergenic RNA-erythroid prosurvival (lincRNA-EPS) is reported to be an effective inhibitor of inflammation, but its role in TMJOA is unexplored. Here, we found that lincRNA-EPS is downregulated and negatively correlated with inflammatory factors in the condyles of TMJOA mice. LincRNA-EPS knockout aggravated inflammation and tissue destruction after TMJOA modeling. The in vitro studies confirmed that loss of lincRNA-EPS facilitated inflammatory factor expression in condylar chondrocytes, while recovered expression of lincRNA-EPS showed anti-inflammatory effects. Mechanistically, RNA sequencing revealed that the inflammatory response pathway nuclear factor-kappa B (NF-κB) was mostly affected by lincRNA-EPS deficiency. Moreover, lincRNA-EPS was proved to effectively bind to serine/arginine-rich splicing factor 3 (SRSF3) and inhibit its function in pyruvate kinase isoform M2 (PKM2) formation, thus restraining the PKM2/NF-κB pathway and the expression of inflammatory factors. In addition, local injection of the lincRNA-EPS overexpression lentivirus significantly alleviated inflammation, cartilage degradation, and subchondral bone loss in TMJOA mice. Overall, lincRNA-EPS regulated the inflammatory process of condylar chondrocytes by binding to SRSF3 and showed translational application potential in the treatment of TMJOA.

Collagen from Iris squid grafted with polyethylene glycol and collagen peptides promote the proliferation of fibroblast through PI3K/AKT and Ras/RAF/MAPK signaling pathways

Collagens from marine sources have been used widely in food, cosmetics and tissue engineering application due to their excellent functional and biological properties. In the present study, a novel protein, collagen from iris squid skin (SSC) was characterized, grafted with polyethylene-glycol (PEG) and Acid-Green 20 (AG) and was investigated the molecular signaling pathways in L-929 fibroblast cells along with their structural peptide analogs. SDS-PAGE and IR spectrum of SSC analysis showed the typical structure of type I collagen. The fibroblast proliferation was evaluated for SSC, SSC grafted PEG (SSC-PEG) and their structural analogs including Gly-Pro-Leu-Gly-Leu-Leu (PEP1), Gly-Pro-Leu-Gly-Leu-Leu-Gly-Phe-Leu (PEP2), Gly-Pro-Leu-Gly-Leu-Leu-Gly-Phe-Leu-Gly-Pro-Leu (PEP3) and Gly-Pro-Leu-Gly-Leu-Leu-Gly-Phe-Leu-Gly-Pro-Leu-Gly-Leu-Ser (PEP4). The optimal concentration of SSC and its derivative was 0.07 μ mol/L. The fibroblast growth-promoting factors were promoted by all the treatment groups by accelerating the PI3K/AKT and Ras/RAF/MAPK signaling pathways in L-929 cells, and inhibiting the secretion of apoptotic factors. Compared to the control group, mRNA and protein expression of AKT in the PI3K/AKT and Ras in Ras/RAF/MAPK signaling pathway were accelerated significantly by PEP4, respectively, while the Bax value was significantly lower (P < 0.01). The promoting effect of PEP1, PEP2, PEP3 and PEP4 on L-929 cells was closely related to the length of the peptides. Therefore, this study disclosed that PEP1, PEP2, PEP3 and PEP4 were novel analogs that greatly promote the proliferation of L-929 cells through PI3K/AKT and Ras/RAF/MAPK signaling pathways.