Femtoscopy using L\'evy-distributed sources at NA61/SHINEIn the recent years, research studies in high-energy physics have confirmed the creation of the strongly interacting quark-gluon plasma (sQGP) in ultra-relativistic nucleus-nucleus collisions.…Barnabas Porfy·Oct 17, 2024SaveLearn
The EMC Effect of Tritium and Helium-3 from the JLab MARATHON ExperimentMeasurements of the EMC effect in the tritium and helium-3 mirror nuclei are reported. The data were obtained by the MARATHON Jefferson Lab experiment, which performed deep inelastic electron…D. Abrams, H. Albataineh, B. S. Aljawrneh et al.·Oct 15, 2024SaveLearn
First constraints on general neutrino interactions based on KATRIN dataThe precision measurement of the tritium β-decay spectrum performed by the KATRIN experiment provides a unique way to search for general neutrino interactions (GNI). All theoretical allowed GNI…M. Aker, D. Batzler, A. Beglarian et al.·Oct 15, 2024SaveLearn
Cluster production in Xe + Sn collisions between 65-150 MeV/nucleonCharacterization of the participant-zone (PZ) in the 129,124Xe + 112,124Sn reaction at the energy range 65-150 MeV/nucleon reveals copious cluster production. A detailed study of the…T. Genard, A. Chbihi, C. Ciampi et al.·Oct 14, 2024SaveLearn
Measurement of Quadrupole Deformation using E2 and M1+E2 Transitions in Heavy Isotopes in the Mass Range of 150<A<250The measurement of a permanent electric dipole moment (EDM) in atoms is crucial for understanding the origins of CP-violation. However, accurate interpretation of the EDM in systems involving…Prajwal MohanMurthy, Lixin Qin, Jeff A. Winger·Oct 11, 2024SaveLearn
Statistical properties and photon strength functions of the 112,114Sn isotopes below the neutron separation thresholdHere, we report on the measurements of the γ-ray strength functions and nuclear level densities of 112,114Sn performed for the first time at the 9~MV Tandem accelerator facilities at…P. -A. Söderström, M. Markova, N. Tsoneva et al.·Oct 9, 2024SaveLearn
High-precision mass measurement of 103Sn restores smoothness of the mass surfaceAs a step towards the ultimate goal of a high-precision mass measurement of doubly-magic 100Sn, the mass of 103Sn was measured at the Low Energy Beam and Ion Trap (LEBIT) located at the…C. M. Ireland, F. M. Maier, G. Bollen et al.·Oct 6, 2024SaveLearn
Correlations between azimuthal anisotropy and mean transverse momentum in pp, pPb, and peripheral PbPb collisionsCorrelations between azimuthal anisotropy and mean transverse momentum of charged particles in proton-proton (pp), proton-lead (pPb), and peripheral lead-lead (PbPb) collisions are presented as a…CMS Collaboration·Oct 6, 2024SaveLearn
Azimuthal Anisotropy Scaling for Identified Mesons and Baryons: Insights into Medium Transport Properties, Equation of State and Hadronic Re-scatteringScaling functions for the centrality and transverse momentum dependence of \(v2(pT,cent)\) and \(v3(pT,cent)\) are constructed for identified mesons and baryons in Pb+Pb…Roy A. Lacey·Oct 6, 2024SaveLearn
Final Results of the MAJORANA DEMONSTRATOR's Search for Double-Beta Decay of 76Ge to Excited States of 76Se76Ge can ββ decay into three possible excited states of 76Se, with the emission of two or, if the neutrino is Majorana, zero neutrinos. None of these six transitions have yet been…I. J. Arnquist, F. T. Avignone, A. S. Barabash et al.·Oct 5, 2024SaveLearn
Light Nuclei Femtoscopy and Baryon Interactions in 3 GeV Au+Au Collisions at RHICWe report the measurements of proton-deuteron (p-d) and deuteron-deuteron (d-d) correlation functions in Au+Au collisions at sNN = 3 GeV using fixed-target mode with the…The STAR Collaboration·Oct 4, 2024SaveLearn
Energy dependence of φ(1020) meson production in nucleus-nucleus collisions at the CERN SPSThis paper presents preliminary results from the NA61/SHINE experiment on φ meson production in central Ar+Sc collisions at beam momenta of 150A, 75A, and 40A GeV/c (corresponding to…Łukasz Rozpłochowski·Oct 3, 2024SaveLearn
Recent J/ measurements at the PHENIX experimentQuarkonium is an ideal probe to explore the properties of quantum chromodynamics (QCD). Unlike Large Hadron Collider (LHC) measurements, quarkonium production at the Relativistic Heavy Ion Collider…Xuan Li·Oct 1, 2024SaveLearn
Electric dipole polarizability of 58NiThe electric dipole strength distribution in 58Ni between 6 and 20 MeV has been determined from proton inelastic scattering experiments at very forward angles at RCNP, Osaka. The experimental…I. Brandherm, F. Bonaiti, P. von Neumann-Cosel et al.·Oct 1, 2024SaveLearn
Precise Mass Measurement of the Longest Odd-Odd Chain of 1+ Ground StatesPrecise mass measurements of the ground and isomeric states of the odd-odd 108, 110, 112, 114, 116Rh were performed using the Canadian Penning Trap at Argonne National Laboratory, showing good…B. Liu, M. Brodeur, J. A. Clark et al.·Oct 1, 2024SaveLearn
Feasibility studies of dark photon searches with the J-PET detectorThe positronium, a bound state of electron and positron is a unique system to perform highly precise tests, due to no hadronic background and precise Quantum Electrodynamics (QED) predictions. Being…Justyna Mędrala-Sowa, Elena Perez del Rio, Wojciech Krzemień·Sep 30, 2024SaveLearn
Assessing the QGP speed of sound in ultra-central heavy-ion collisions with ALICEUltrarelativistic heavy-ion collisions produce a state of hot, dense, strongly interacting QCD matter known as quark-gluon plasma (QGP). On an event-by-event basis, the volume of the QGP in…Omar Vazquez Rueda·Sep 30, 2024SaveLearn
K*/K ratio and the time between freeze-outs for intermediate-mass Ar+Sc system at the SPS energy rangeResonance production is one of the key observables to study the dynamics of high-energy collisions. In dense systems created in heavy nucleus-nucleus collisions, the properties of some of them…Bartosz Kozłowski·Sep 30, 2024SaveLearn
Recent results from NA61/SHINEThe NA61/SHINE experiment at the CERN SPS is a multipurpose fixed-target spectrometer for charged and neutral hadron measurements. Its research program includes studies of strong interactions as well…Andrzej Rybicki·Sep 29, 2024SaveLearn
Clocking the particle production and tracking of strangeness balance and radial flow effects at top LHC energy with ALICEBalance functions have been used extensively to elucidate the time evolution of quark production in heavy-ion collisions. Early models predicted two stages of quark production, one for light quarks…Victor Gonzalez·Sep 27, 2024SaveLearn
Charged-particle production in pp collisions at s = 13.6 TeV and Pb-Pb collisions at sNN = 5.36 TeV with ALICEThis article presents the measurement of charged-particle pseudorapidity (η) density, dN ch/dη, in proton-proton (pp) collisions at a centre-of-mass energy…Abhi Modak·Sep 27, 2024SaveLearn
First Measurement of Near- and Sub-Threshold J/ Photoproduction off NucleiWe report on the first measurement of J/ photoproduction from nuclei in the photon energy range of 7 to 10.8 GeV, extending above and below the photoproduction threshold in the free proton…J. R. Pybus, L. Ehinger, T. Kolar et al.·Sep 27, 2024SaveLearn
The glue that binds us all -- Latin America and the Electron-Ion ColliderThe Electron-Ion Collider, a next generation electron-hadron and electron-nuclei scattering facility, will be built at Brookhaven National Laboratory. The wealth of new data will shape research in…A. C. Aguilar, A. Bashir, J. J. Cobos-Martínez et al.·Sep 27, 2024SaveLearn
Remeasurement of the 239Pu(n,f)/235U(n,f) Cross-Section Ratio with the NIFFTE fission Time Projection Chamber Using Vapor-deposited TargetsThe NIFFTE fission Time Projection Chamber (fissionTPC) has been used to measure the 239Pu(n,f)/235U(n,f) cross-section ratio for neutron-induced fission in the range of 0.1 - 100 MeV, with…D. H. Dongwi, L. Snyder, V. Aguilar et al.·Sep 26, 2024SaveLearn
Temperature dependent ultracold neutron transmission in D2 gas - a test of the Young-Koppel modelThe Young-Koppel model (YK) describes comprehensively the interaction of slow neutrons with diatomic gases such as H2 and D2. This paper reports on the first experimental results of ultracold…G. Bison, R. Grössle, K. Kirch et al.·Sep 26, 2024SaveLearn