Effects of centrality fluctuation and deuteron formation on proton number cumulant in Au+Au collisions at sNN = 3 GeV from JAM modelWe studied the effects of centrality fluctuation and deuteron formation on the cumulants (Cn) and correlation functions (n) of protons up to sixth order in most central (b<3 fm) Au+Au…Arghya Chatterjee, Yu Zhang, Hui Liu et al.·Sep 8, 2020SaveLearn
Precision measurements of A=3 nuclei in Hall BWe propose a high-statistics measurement of few body nuclear structure and short range correlations in quasi-elastic scattering at 6.6 GeV from 2H, 3He and 3H targets in Hall B with the…Or Hen, Dave Meekins, Dien Nguyen et al.·Sep 7, 2020SaveLearn
Light meson nuclear modification factor in p-Pb collisions over an unprecedented pT range with ALICELight neutral meson differential invariant cross section and nuclear modification factor measurements have been carried out with the ALICE detector at the CERN LHC in pp collisions at s=8…Nicolas Schmidt·Sep 7, 2020SaveLearn
A Proposed Forward Silicon Tracker for the Future Electron-Ion Collider and Associated Physics StudiesThe future Electron-Ion Collider (EIC) will explore several fundamental questions in a broad Bjorken-x (xBJ) and Q2 phase space. Heavy flavor and jet products are ideal probes to precisely…Cheuk-Ping Wong, Xuan Li, Melynda Brooks et al.·Sep 7, 2020SaveLearn
Recent progress in multiple chiral doublet bandsThe recent progress of multiple chiral doublet bands (M) is reviewed for both experimental and theoretical sides. In particular, the experimental findings, theoretical predictions, selection…Shou-Yu Wang·Sep 7, 2020SaveLearn
Measurements of natPb(p,xn)201-207Bi, 204Pb(p,1-4n)201-204Bi and 206Pb(p,3n)204Bi cross-sections at astrophysical energies (Ep ≤ 30 \, MeV)Cross-sections for natPb(p,xn)201-207Bi, 204Pb(p,1-4n)201-204Bi and 206Pb(p,3n)204Bi reactions have been determined in the astrophysical energy range $20-30 \,…P V Guillaumon, I D Goldman, V R Vanin et al.·Sep 7, 2020SaveLearn
Measurements of heavy-flavor jets with ALICE at the LHCHeavy quarks created in ultra-relativistic heavy-ion collisions are mostly produced in hard QCD processes during the early stages of the reaction. They interact with the hot and cold nuclear matter…Ashik Ikbal Sheikh·Sep 6, 2020SaveLearn
Investigation of the elliptic flow fluctuations of the identified particles using the A Multi-Phase Transport modelA Multi-Phase Transport (AMPT) model is used to study the elliptic flow fluctuations of identified particles using participant and spectator event planes. The elliptic flow measured using the first…Niseem Magdy, Xu Sun, Zhenyu Ye et al.·Sep 6, 2020SaveLearn
Evidence for top quark production in nucleus-nucleus collisionsUsing 1.7 0.1\,nb-1 of lead-lead (A = 208) collision data recorded by the CMS experiment at a nucleon-nucleon center-of-mass energy of 5.02 TeV, we report evidence of top quark…Georgios Konstantinos Krintiras·Sep 4, 2020SaveLearn
Inclusive Jet Measurements in Pb-Pb Collisions at 5.02 TeV with ALICE using Machine Learning TechniquesThese proceedings report on measurements of the jet spectrum and nuclear modification factor for inclusive full jets (containing both charged and neutral constituents) in Pb-Pb and pp collisions at…Hannah Bossi·Sep 4, 2020SaveLearn
Manifestation of one- and two-body currents in longitudinal and transverse response functions of the 12C nucleus at q = 300 MeV/cThe experimental values of longitudinal and transverse response functions of the 12C nucleus have been obtained at the 3-momentum transfer q = 300 MeV/c. The data are compared with the calculations…A. Yu. Buki, I. S. Timchenko·Sep 4, 2020SaveLearn
Measurements of multiplicity fluctuations of identified hadrons in inelastic proton-proton interactions at the CERN Super Proton SynchrotronMeasurements of multiplicity fluctuations of identified hadrons produced in inelastic p+p interactions at 31, 40, 80, and 158~ beam momentum are presented. Three different measures of…SHINE Collaboration, A. Acharya, H. Adhikary et al.·Sep 3, 2020SaveLearn
Status of CME Search Before Isobar Collisions and Methods of Blind Analysis From STARThe STAR collaboration is currently pursuing the blind analysis of the data for isobar collisions that was performed at RHIC in the year 2018 to make a decisive test of the Chiral Magnetic Effect…Prithwish Tribedy·Sep 3, 2020SaveLearn
Search for alpha decay of naturally occurring osmium nuclides accompanied by gamma quantaA search for α decay of naturally occurring osmium isotopes to the lowest excited levels of daughter nuclei has been performed by using an ultra-low-background Broad-Energy Germanium…P. Belli, R. Bernabei, F. Cappella et al.·Sep 3, 2020SaveLearn
Centrality determination with a forward detector in the RHIC Beam Energy ScanRecently, Chatterjee et al used a hadronic transport model to estimate the resolution with which various experimental quantities select the impact parameter of relativistic heavy ion collisions at…Skipper Kagamaster, Rosi Reed, Michael Lisa·Sep 3, 2020SaveLearn
Accessing the Single-Particle Structure of the Pygmy Dipole Resonance in 208PbNew experimental data on the neutron single-particle character of the Pygmy Dipole Resonance (PDR) in 208Pb are presented. They were obtained from (d,p) and resonant proton scattering…M. Spieker, A. Heusler, B. A. Brown et al.·Sep 2, 2020SaveLearn
The percolation phase transition and statistical multifragmentation in finite systemsThe cumulant ratios up to fourth order of the Z distributions of the largest fragment in spectator fragmentation following 107,124Sn+Sn and 124La+Sn collisions at 600 MeV/nucleon have…T. Pietrzak, A. S. Botvina, J. Brzychczyk et al.·Sep 2, 2020SaveLearn
Estimation of CP violating EDMs from known mechanisms in the SMNew sources of CP violation, beyond the known sources in the standard model (SM), are required to explain the baryon asymmetry of the universe. Measurement of a non-zero permanent electric dipole…Prajwal Mohanmurthy, Jeff A. Winger·Sep 2, 2020SaveLearn
25Si β+-decay spectroscopyβ-decay spectroscopy provides valuable information on exotic nuclei and a stringent test for nuclear theories beyond the stability line. To search for new β-delayed protons and γ…L. J. Sun, M. Friedman, T. Budner et al.·Sep 2, 2020SaveLearn
Shell structure of 43S and collapse of the N=28 shell closureThe single-particle structure of the N=27 isotones provides insights into the shell evolution of neutron-rich nuclei from the doubly-magic 48Ca toward the drip line. 43S was studied…S. Momiyama, K. Wimmer, D. Bazin et al.·Sep 2, 2020SaveLearn
First Observation of Multiple Transverse Wobbling Bands of Different Kinds in 183AuWe report the first observation of two wobbling bands in 183Au, both of which were interpreted as the transverse wobbling (TW) band but with different behavior of their wobbling energies as a…S. Nandi, G. Mukherjee, Q. B. Chen et al.·Sep 1, 2020SaveLearn
A comprehensive analysis of differential cross sections and analyzing powers in the proton-deuteron break-up channel at 135 MeVA selection of measured cross sections and vector analyzing powers, Ax and Ay, are presented for the pd break-up reaction. The data are taken with a polarized proton beam energy of 135 MeV using the…H. Tavakoli-Zaniani, M. Eslami-Kalantari, H. R. Amir-Ahmadi et al.·Aug 27, 2020SaveLearn
Determination of luminosity for in-ring reactions: A new approach for the low-energy domainLuminosity is a measure of the colliding frequency between beam and target and it is a crucial parameter for the measurement of absolute values, such as reaction cross sections. In this paper, we…Y. M. Xing, J. Glorius, L. Varga et al.·Aug 27, 2020SaveLearn
Measurement of the high-energy contribution to the Gerasimov-Drell-Hearn sum ruleWe propose to measure the high-energy behavior of the integrand of the Gerasimov-Drell-Hearn (GDH) sum rule on the proton and the neutron up to 12 GeV. The convergence of the GDH integral will be…M. M. Dalton, A. Deur, C. D. Keith et al.·Aug 25, 2020SaveLearn
Backward-angle Exclusive pi0 Production above the Resonance RegionThe proposed measurement is a dedicated study of the exclusive electroproduction process,1H(e,e'p)pi0, in the backward-angle regime (u-channel process) above the resonance region. The produced pi0 is…W. B. Li, G. M. Huber, J. R. Stevens et al.·Aug 25, 2020SaveLearn