Exploring Electromagnetic Field Effects and Constraining Transport Parameters of QGP using STAR BES-II dataHeavy-ion collisions undergo various stages in their evolution and it is crucial to disentangle the initial- and final-stage effects. In this work, we report measurements of two types of observables:…Aditya Prasad Dash·Jan 9, 2024SaveLearn
Insight into Emergence of Hadron Mass from N* Electroexcitation AmplitudesThe emergence of hadron mass represents one of the most challenging and still open problems in contemporary hadron physics. The results on the nucleon resonance electroexcitation amplitudes available…V. I. Mokeev, D. S. Carman·Jan 9, 2024SaveLearn
Results of the MAJORANA DEMONSTRATOR's Search for Neutrinoless Double Beta DecayThe MAJORANA DEMONSTRATOR recently concluded its search for neutrinoless double-beta decay. The experiment operated an array of up to 40.4 kg of germanium detectors, 27 kg of which were isotopically…David J. Tedeschi·Jan 9, 2024SaveLearn
Interaction of photons with silver and indium nuclei at energies up to 20 MeVThe yields of photonuclear reactions in the 107Ag, 113In, and 115In nuclei have been measured. Monte Carlo simulations have been performed using the Geant4 code, and the results have been compared…J. H. Khushvaktov, M. A. Demichev, D. L. Demin et al.·Jan 9, 2024SaveLearn
Cross-shell excited configurations in the structure of 34SiThe cross-shell excited states of 34Si have been investigated via β-decays of the 4- ground state and the 1+ isomeric state of 34Al. Since the valence protons and valence…R. S. Lubna, A. B. Garnsworthy, Vandana Tripathi et al.·Jan 8, 2024SaveLearn
Measurement of 144Sm(p,γ) cross-section at Gamow energiesThe cross-section measurement of 144Sm(p, γ)145Eu (T1/2=5.93(4) days) reaction has been performed at proton energies around 2.6, 3.1, 3.7, 4.1, 4.2, 4.7, 5.1, 5.5, 5.9, 6.4, 6.8…Tanmoy Bar, Dipali Basak, Lalit Kumar Sahoo et al.·Jan 7, 2024SaveLearn
Search for a critical point of strongly-interacting matter in central 40Ar +45Sc collisions at 13A-75A GeV/c beam momentumThe critical point of strongly interacting matter is searched for at the CERN SPS by the NA61/SHINE experiment in central 40Ar +45Sc collisions at 13A, 19A, 30A, 40A, and 75A…SHINE Collaboration, H. Adhikary, P. Adrich et al.·Jan 7, 2024SaveLearn
Femtoscopy analysis in small systems at NA61/SHINERecent measurements of femtoscopic correlations at NA61/SHINE unravel that the shape of the particle emitting source is not Gaussian. The measurements are based on L\'evy-stable symmetric sources,…Barnabas Porfy·Jan 4, 2024SaveLearn
Measurements of p- and d- correlations in 3 GeV Au+Au collisions at STARHeavy-ion collisions provide a unique opportunity to explore nucleon-hyperon (N-Y) interactions through two-particle correlations. The p- and d- correlations shed light on both N-Y…Yu Hu·Dec 30, 2023SaveLearn
Search for the Chiral Magnetic and Vortical Effects Using Event Shape Approaches in Au+Au Collisions at STARThe chiral magnetic/vortical effect (CME/CVE) in heavy-ion collisions probe the topological sector of Quantum Chromodynamics, where P and CP symmetries are violated locally in strong interactions.…Zhiwan Xu·Dec 30, 2023SaveLearn
Population of tetraneutron continuum in reactions of 8He on deuteriumSearch for the population of the low-energy continuum of a tetraneutron system was performed for reactions of the 8He beam on a deuterium target. These studies are based on the data [I.A.…I. A. Muzalevskii, N. B. Shulgina, A. A. Bezbakh et al.·Dec 28, 2023SaveLearn
Elliptic anisotropy measurement of the f0(980) hadron in proton-lead collisions and evidence for its quark-antiquark compositionDespite the f0(980) hadron having been discovered half a century ago, the question about its quark content has not been settled: it might be an ordinary quark-antiquark (qq)…CMS Collaboration·Dec 28, 2023SaveLearn
Search for the 6α condensed state in 24Mg using the 12C+12C scatteringWe searched for the 6α-condensed state in 24Mg by measuring the 12C+12C scattering with the SAKRA Si detector array at Ecm = 17.5-25.0 MeV. By using the…Y. Fujikawa, T. Kawabata, S. Adachi et al.·Dec 28, 2023SaveLearn
Anisotropic Flow of Identified Particles in Au + Au Collisions at sNN = 3-3.9 GeV at RHICIn these proceedings, we present transverse momentum dependence of the mid-rapidity slope of directed flow (dv1/dy|y=0) for π+ and KS0 in Au + Au collisions at sNN = 3.0,…Zuowen Liu·Dec 28, 2023SaveLearn
New Experimental Opportunities in Spin-Physics for Meson BeamsDuring the past several decades a large quantity of high-quality mesonic photo- and electro- production data have been measured at electromagnetic facilities worldwide. By contrast, meson-beam data…William J. Briscoe, Igor I. Strakovsky·Dec 26, 2023SaveLearn
Hypertriton Production in Au+Au Collisions from STAR BES-IIHypernuclei are bound states of nuclei with one or more hyperons. Precise measurements of hypernuclei properties and their production yields in heavy ion collisions are crucial for the understanding…Yuanjing Ji·Dec 25, 2023SaveLearn
New Insights into Global Spin Alignment of Vector Mesons Using Relativistic Heavy-Ion Collisions from STARIn these proceedings, we present new measurements from STAR of the global spin alignment(00) of φ mesons in Au+Au collisions at sNN = 19.6, 14.6 GeV using BES-II…Baoshan Xi·Dec 25, 2023SaveLearn
Searching for Two-Neutrino and Neutrinoless Double Beta Decay of 134Xe with the PandaX-4T Experiment134Xe is a candidate isotope for neutrinoless double beta decay~(0ββ) search. In addition, the two-neutrino case (2ββ) allowed by the Standard Model of particle physics…PandaX Collaboration, Xiyu Yan, Zhaokan Cheng et al.·Dec 25, 2023SaveLearn
Measurements of c+ /D0 ratio as a function of multiplicity at midrapidity at sNN = 5.02\; TeVIn this contribution, the measurement of prompt c+ /D0 ratio as a function of multiplicity in p--Pb collisions at mid-rapidity at sNN = 5.02 \;TeV is…Oveis Sheibani·Dec 24, 2023SaveLearn
Photonuclear reaction in 67ZnMono-energetic γ-beams ( ≈ 10 eV) based on thermal neutron capture, in a nuclear reactor, using the Mn(n, γ) reaction were utilized for generating a fast neutron source…Sylvian Kahane, Raymond Moreh·Dec 22, 2023SaveLearn
First measurement of the neutron-emission probability with a surrogate reaction in inverse kinematics at a heavy-ion storage ringNeutron-induced reaction cross sections of short-lived nuclei are imperative to understand the origin of heavy elements in stellar nucleosynthesis and for societal applications, but their measurement…M. Sguazzin, B. Jurado, J. Pibernat et al.·Dec 21, 2023SaveLearn
Impact of the MARATHON data on F2n/F2pF2n/F2p and off-shell effects in light nucleiThe neutron structure function, F2n, has historically been extracted from measurements of the deuteron structure function, but our understanding of the nuclear effects on the bound proton and…T. J. Hague, J. Arrington, S. Li et al.·Dec 21, 2023SaveLearn
Quarkonia as probes of initial and final states in small systems with ALICEThe multiple parton-parton interactions (MPIs) are an important element to describe the observed collective flow and strangeness enhancement in high multiplicity pp and p-Pb collisions, the…Subikash Choudhury·Dec 20, 2023SaveLearn
Measurements of azimuthal anisotropies in 16O+16O and γ+Au collisions from STARIn this proceeding, we present the first measurements of azimuthal anisotropies, v2 and v3, in 16O+16O collisions at 200 GeV as a function of transverse momentum and multiplicity, by…Shengli Huang·Dec 19, 2023SaveLearn
Anti-deuteron beam study at J-PARC HEF K1.8 beam lineWe performed a d beam study at the K1.8 beam line of J-PARC Hadron Experimental Facility. 1.8 GeV/c d beam yield was measured to be 0.30 0.04 counts/spill for 30 GeV…M. Ukai, Y. Ishikawa, T. Takahashi et al.·Dec 19, 2023SaveLearn