Photonuclear reactions 65Cu(γ,n)64Cu and 63Cu(γ,xn)63-xCu cross-sections in the energy range Eγ max = 35-94 MeVThe bremsstrahlung flux-averaged cross-sections σ(Eγ max) for the photonuclear reactions 65Cu(γ,n)64Cu,…O. S. Deiev, I. S. Timchenko, S. M. Olejnik et al.·May 29, 2022SaveLearn
(1385) resonance production in Pb-Pb collisions at sNN=5.02 TeVHadronic resonances are used to probe the hadron gas produced in the late stage of heavy-ion collisions since they decay on the same timescale, of the order of 1 to 10 fm/c, as the decoupling time…ALICE Collaboration·May 27, 2022SaveLearn
First measurement of c0 production in pp collisions at s=13 TeVThe inclusive production of the charm-strange baryon c0 is measured for the first time via its hadronic decay into -π+ at midrapidity (|y|<0.5) in proton-proton (pp)…ALICE Collaboration·May 27, 2022SaveLearn
Constraints on the onset of color transparency from quasi-elastic 12C(e,e'p) up to Q2=\,14.2\,(GeV/c)2Quasi-elastic scattering on 12C(e,e'p) was measured in Hall C at Jefferson Lab for space-like 4-momentum transfer squared Q2 in the range of 8--14.2\,(GeV/c)2 with proton momenta up to…D. Bhetuwal, J. Matter, H. Szumila-Vance et al.·May 26, 2022SaveLearn
Measurement of Double Beta Decay Half-life of 136Xe with the PandaX-4T DetectorPrecise measurement of two-neutrino double beta decay (DBD) half-life is an important step for the searches of Majorana neutrinos with neutrinoless double beta decay. We report the measurement of DBD…PandaX Collaboration, Lin Si, Zhaokan Cheng et al.·May 25, 2022SaveLearn
Accessing DEMP and DVCS at Backward Angles above the Resonance RegionThe proposed measurement is a dedicated study to investigate the exclusive electroproduction process: 1H(e, e'p)X, in the backward angle above the resonance region. Here, the produced particle X (pi0…W. B. Li, J. R. Stevens, G. M. Huber·May 24, 2022SaveLearn
Precision Determination of the Neutral Weak Form Factor of 48CaWe report a precise measurement of the parity-violating asymmetry A PV in the elastic scattering of longitudinally polarized electrons from 48 Ca. We measure $A PV =2668…D. Adhikari, H. Albataineh, D. Androic et al.·May 23, 2022SaveLearn
Azimuthal anisotropy measurement of (multi-)strange hadrons in Au+Au collisions at sNN = 54.4 GeVAzimuthal anisotropy of produced particles is one of the most important observables used to access the collective properties of the expanding medium created in relativistic heavy-ion collisions. In…STAR Collaboration, M. S. Abdallah, B. E. Aboona et al.·May 23, 2022SaveLearn
Search for Neutrinoless Double-Beta Decay of 76Ge with a Natural Broad Energy Germanium DetectorA natural broad energy germanium (BEGe) detector is operated in the China Jinping Underground Laboratory (CJPL) for a feasibility study of building the next generation experiment of the neutrinoless…CDEX collaboration, W. H. Dai, H. Ma et al.·May 22, 2022SaveLearn
Direct determination of the excitation energy of quasi-stable isomer 180mTa180mTa is a naturally abundant quasi-stable nuclide and the longest-lived nuclear isomer known to date. It is of interest for, among others, the search for dark matter, for the development of a…D. A. Nesterenko, K. Blaum, P. Delahaye et al.·May 21, 2022SaveLearn
Proton Compton Scattering from Linearly Polarized Gamma RaysDifferential cross sections for Compton scattering from the proton have been measured at scattering angles of 55, 90, and 125 in the laboratory frame using quasimonoenergetic…X. Li, M. W. Ahmed, A. Banu et al.·May 21, 2022SaveLearn
First results from the INDRA-FAZIA apparatus on isospin diffusion in 58,64Ni+58,64Ni systems at Fermi energiesAn investigation of the isospin equilibration process in the reactions 58,64Ni+58,64Ni at two bombarding energies in the Fermi regime (32\,MeV/nucleon and 52\,MeV/nucleon) is presented.…C. Ciampi, S. Piantelli, G. Casini et al.·May 20, 2022SaveLearn
Feasibility of studying astrophysically important charged-particle emission with the variable energy γ-ray system at the Extreme Light Infrastructure -- Nuclear Physics facilityIn the environment of a hot plasma, as achieved in stellar explosions, capture and photodisintegration reactions proceeding on excited states in the nucleus can considerably contribute to the…H. Y. Lan, W. Luo, Y. Xu et al.·May 19, 2022SaveLearn
Emergence of an island of extreme nuclear isomerism at high excitation near 208PbMetastable states with T1/2 = 8(2) ms in 205Bi and T1/2 = 0.22(2) ms in 204Pb, with ≈ 8 MeV excitation energy and angular momentum 22 , have been…S. G. Wahid, S. K. Tandel, Saket Suman et al.·May 19, 2022SaveLearn
Proton capture on 30P in novae: On the existence of states at 6.40 MeV and 6.65 MeV in 31SWe use a high resolution 32 S(d,t) measurement to investigate the claimed existence of a 6401(3) keV state in 31S that may affect the 30 P(p,γ) nuclear reaction rate in…M. Kamil, S. Triambak, G. C. Ball et al.·May 17, 2022SaveLearn
Horizons: Nuclear Astrophysics in the 2020s and BeyondNuclear Astrophysics is a field at the intersection of nuclear physics and astrophysics, which seeks to understand the nuclear engines of astronomical objects and the origin of the chemical elements.…H. Schatz, A. D. Becerril Reyes, A. Best et al.·May 16, 2022SaveLearn
Observation of the X17 anomaly in the 7Li(p,e+e-)8Be direct proton-capture reactionAngular correlation spectra of e+e- pairs produced in the 7Li(p,γ)8Be nuclear reaction have been studied at the sharp Ep= 441 keV resonance as well as at Ep= 650 keV, 800…N. J. Sas, A. J. Krasznahorkay, M. Csatlós et al.·May 16, 2022SaveLearn
Thermonuclear reaction rate of 29Si(p,γ)30PThe thermonuclear rate of the 29Si(p,γ)30P reaction impacts the 29Si abundance in classical novae. A reliable reaction rate is essential for testing the nova paternity of…Lori Downen, Christian Iliadis, Art Champagne et al.·May 13, 2022SaveLearn
Electric monopole transition from the superdeformed band in 40CaThe electric monopole (E0) transition strength 2 for the transition connecting the third 0+ level, a "superdeformed" band head, to the "spherical" 0+ ground state in doubly magic…E. Ideguchi, T. Kibédi, J. T. H. Dowie et al.·May 13, 2022SaveLearn
Analysis of 2-Body Central Events for 129Xe+natSn from 8A MeV up to 18A MeV and for 129Xe+197Au at 15A MeV and 18A MeVA study of medium-mass heavy-ion reactions leading to two fragments in the exit channel from barrier to 18A MeV is proposed. A special focus is made on fission and quasi-fission for events with two…L. Manduci, O. Lopez, D. Durand et al.·May 12, 2022SaveLearn
Search for neutrinoless quadruple beta decay of 136Xe in XMASS-IA search for the neutrinoless quadruple beta decay of 136Xe was conducted with the liquid-xenon detector XMASS-I using 327\; kg × 800.0 \; days of the exposure. The pulse shape…XMASS Collaboration, K. Abe, K. Hiraide et al.·May 11, 2022SaveLearn
Evidence of a near-threshold resonance in 11B relevant to the β-delayed proton emission of 11BeA narrow near-threshold proton-emitting resonance (Ex = 11.4 MeV, Jπ = 1/2+ and p = 4.4 keV) was directly observed in 11B via proton resonance scattering. This resonance…Y. Ayyad, W. Mittig, T. Tang et al.·May 10, 2022SaveLearn
First results of the nuGeN experiment on coherent elastic neutrino-nucleus scatteringThe nuGeN experiment is aimed to investigate neutrino properties using antineutrinos from the reactor of the Kalinin Nuclear Power Plant. The experimental setup is located at about 11 meters from the…I. Alekseev, K. Balej, V. Belov et al.·May 9, 2022SaveLearn
Measurement of the prompt D0 nuclear modification factor in pPb collisions at sNN = 8.16 TeVThe production of prompt D0 mesons in proton-lead collisions in the forward and backward configurations at a center-of-mass energy per nucleon pair of sNN = 8.16~TeV is…LHCb collaboration·May 8, 2022SaveLearn
New direct limit on neutrinoless double beta decay half-life of 128Te with CUOREThe Cryogenic Underground Observatory for Rare Events (CUORE) at Laboratori Nazionali del Gran Sasso of INFN in Italy is an experiment searching for neutrinoless double beta (0ββ) decay.…D. Q. Adams, C. Alduino, K. Alfonso et al.·May 6, 2022SaveLearn