Cross-section of the natNi(γ, p x n)58Co reaction at the bremsstrahlung end-point energy of 35-94 MeVThe photoproduction of the 58Co nuclei on natNi was studied using the induced γ-activity method and off-line γ-ray spectrometric technique. The experiment was…I. S. Timchenko, O. S. Deiev, S. M. Olejnik et al.·May 15, 2025SaveLearn
Rapidity and multiplicity dependence of charged-particle flow in pPb collisions at sNN = 8.16 TeVThe elliptic and triangular flow of charged particles are measured using two-particle angular correlations in pPb collisions in the pseudorapidity range 2.0 < |η| < 4.8. The data sample…R. Aaij, A. S. W. Abdelmotteleb, C. Abellan Beteta et al.·May 14, 2025SaveLearn
Heavy-Ion and Fixed-Target Physics at LHCbThe LHCb experiment, designed for searches of new physics in beauty and charm hadron decays, has been recording data at the Large Hadron Collider since 2010. The physics program incorporates pp,…Krista Smith·May 14, 2025SaveLearn
Measurement of the Total Compton Scattering Cross Section between 6.5 and 11 GeVThe total cross section for Compton scattering off atomic electrons, γ+e→γ'+e', was measured using photons with energies between 6.5 and 11.1 GeV incident on a 9Be target as…GlueX Collaboration, F. Afzal, C. S. Akondi et al.·May 12, 2025SaveLearn
Extraction of the non-spin- and spin-transfer isovector responses via the 12C(10Be,10B+γ)12B reactionThe isovector response in 12B was investigated via the 12C(10Be,10B+γ)12B reaction at 100 A \, MeV. By utilizing the γ-decay…Sk M. Ali, C. Maher, R. G. T. Zegers et al.·May 10, 2025SaveLearn
The 76Cu conundrum remains unsolvedNear the doubly-magic nucleus Ni78 (Z=28, N=50), there has been a decades-long debate on the existence of a long-lived isomer in Cu76. A recent mass measurement claimed to have…B. Olaizola, A. Illana, J. Benito et al.·May 9, 2025SaveLearn
Dielectron measurements in Au+Au collisions at BES-II energies with the STAR experimentDielectrons, emitted during the evolution of the hot and dense QCD medium created in relativistic heavy-ion collisions, offer an effective probe of the hot medium properties, as they do not involve…Chenliang Jin·May 9, 2025SaveLearn
Robust Method for Confidence Interval Estimation in Outlier-Prone Datasets: Application to Molecular and Biophysical DataEstimating confidence intervals in small or noisy datasets is a challenge in biomolecular research when data contain outliers or high variability. We introduce a robust method combining a hybrid…Victor V. Golovko·May 9, 2025SaveLearn
Study of beta spectrum shapes relevant to the prediction of reactor antineutrino spectraThe shapes of the beta spectra of 92Rb and 142Cs, two of the beta decays most relevant for the prediction of the antineutrino spectrum in reactors, have been measured. A new setup composed of two…G. A. Alcalá, A. Algora, M. Estienne et al.·May 9, 2025SaveLearn
Artificial intelligence pioneers the double-strangeness factoryArtificial intelligence (AI) is transforming not only our daily experiences but also the technological development landscape and scientific research. In this study, we pioneered the application of AI…Yan He, Takehiko R. Saito, Hiroyuki Ekawa et al.·May 9, 2025SaveLearn
Measurement of medium-induced acoplanarity in central Au-Au and pp collisions at s NN=200 GeV using direct-photon+jet and π0+jet correlationsThe STAR Collaboration reports measurements of acoplanarity using semi--inclusive distributions of charged--particle jets recoiling from direct photon and π0 triggers, in central Au+Au and…The STAR Collaboration·May 9, 2025SaveLearn
Gluonic Energy Momentum Tensor Form Factors of the ProtonGravitational form factors (GFFs), defined through the matrix elements of the energy-momentum tensor, provide critical insights into the internal structure of nucleons and nuclei. In particular,…Zein-Eddine Meziani·May 8, 2025SaveLearn
Hyperon global polarization in isobar Ru+Ru and Zr+Zr collisions at sNN = 200 GeVThe polarization of Lambda, Anti-Lambda, Xi, and Anti-Xi hyperons along the angular momentum of the system has been measured in isobar collisions of Ru+Ru and Zr+Zr at sNN = 200 GeV with…The STAR Collaboration·May 8, 2025SaveLearn
Total cross section of 14N+n from 0.1 to 12~MeVThe reaction 14N(n,p)14C is one of the main neutron poisons during s-process nucleosynthesis. In addition, the reaction provides insight into the yields of atmospheric nuclear weapon…R. J. deBoer, R. Arquette, D. Bemmerer et al.·May 8, 2025SaveLearn
Jet Quenching in Heavy-Ion Collisions at RHIC and the LHC experimentsJet quenching serves as a key probes of the Quark-Gluon Plasma (QGP) in heavy-ion collisions. This proceedings presents recent results from RHIC and LHC on jet energy loss, acoplanarity, and the…Nihar Ranjan Sahoo·May 7, 2025SaveLearn
Proceedings of Direct photon measurement in small systems and thermal radiation from QGP with ALICE, Hard Probes conference 2024Electromagnetic probes are a unique tool for studying the space-time evolution of the hot and dense matter created in ultra-relativistic heavy-ion collisions. Dielectrons are emitted during the…Jerome Jung·May 6, 2025SaveLearn
Uranium and Plutonium antineutrino spectra taken by summation method used to fit experimentally measured reactor antineutrino spectrumAntineutrino spectra of fissile isotopes calculated using summation method being used to fit experimental spectra got in several experiments. Summation method was used with the possibility of…Valery Sinev, Pavel Alzhev, Svetlana Ingerman et al.·May 4, 2025SaveLearn
The NA60+ experiment at SPSA new apparatus, NA60+, is proposed for measuring muon pairs in the center-of-mass region from 5 to 17 GeV at CERN SPS in various collisional systems from Pb+Pb and down to p+Be. The physics scope…Alexander Milov·May 4, 2025SaveLearn
28Al Half-life Measurement and the negative mirror asymmetry between the 28Al(β-)28mSi and 28P(β+)28mSi decaysIn the past, the mirror asymmetry parameter has been proposed as a probing mechanism for the presence of beyond the Standard Model second-class currents in nuclear beta decay transitions. However,…B. Liu, M. Brodeur, D. W. Bardayan et al.·May 3, 2025SaveLearn
Femtoscopic study of the proton-proton and proton-deuteron systems in heavy-ion collisions at the LHCThis work reports femtoscopic correlations of p-p ( p- p) and p-d ( p- d) pairs measured in Pb-Pb collisions at center-of-mass energy per nucleon…ALICE Collaboration·May 2, 2025SaveLearn
Measuring 241Am Dipole ResponseAmericium (241Am) with an unpaired proton in the F5/2 state exhibits a significant magnetic dipole moment. The dipole can be experimentally measured with application of even modest external…C. Scarlett, E. Fischbach, B. Freeman et al.·May 1, 2025SaveLearn
Hard-jet correlations in large and small systemsHard-jet correlations probe parton energy loss and the microscopic structure of the quark-gluon plasma formed in ultra-relativistic heavy-ion collisions. The correlation of high-pT jets…Riccardo Longo·May 1, 2025SaveLearn
Potential for Tensor Polarized Deuterons in Hall D at Jefferson LabHall D at Jefferson lab is an ideal place to install a polarized deuteron target which can be ''tensor polarized", allowing the separation of the spin states m=0,1 or the measurement of tensor…Mark M. Dalton, Alexandre Deur, Chris Keith·Apr 29, 2025SaveLearn
Measurement of single- and double-polarization observables in the photoproduction of π+π-~meson pairs off the proton using CLAS at Jefferson LaboratoryThe photoproduction of π+π- meson pairs off the proton has been studied in the reaction γ p p\,π+π- using the CEBAF Large Acceptance Spectrometer (CLAS) and the frozen-spin…P. Roy, S. Cao, V. Crede et al.·Apr 29, 2025SaveLearn
Probing Quantum Phenomena through Photoproduction in Relativistic Heavy-Ion CollisionsPhotoproduction in ultra-peripheral relativistic heavy-ion collisions displays many unique features, often involving quantum mechanical coherence and two-source interference between photon emission…James Daniel Brandenburg, Spencer R. Klein, Zhangbu Xu et al.·Apr 25, 2025SaveLearn