Tritium Beta Spectrum and Neutrino Mass Limit from Cyclotron Radiation Emission SpectroscopyThe absolute scale of the neutrino mass plays a critical role in physics at every scale, from the particle to the cosmological. Measurements of the tritium endpoint spectrum have provided the most…Project 8 Collaboration, A. Ashtari Esfahani, S. Böser et al.·Dec 9, 2022SaveLearn
High-resolution laser system for the S3-Low Energy BranchIn this paper we present the first high-resolution laser spectroscopy results obtained at the GISELE laser laboratory of the GANIL-SPIRAL2 facility, in preparation for the first experiments with the…Jekabs Romans, Anjali Ajayakumar, Martial Authier et al.·Dec 9, 2022SaveLearn
Measurement of the production of (anti)nuclei in p-Pb collisions at s NN = 8.16 TeVMeasurements of (anti)proton, (anti)deuteron, and (anti)3He production in the rapidity range -1<y< 0 as a function of the transverse momentum and event multiplicity in p-Pb collisions at a…ALICE Collaboration·Dec 9, 2022SaveLearn
54Fe(d,p)55Fe and the evolution of single neutron energies in the N=29 isotonesA measurement of the 54Fe(d,p)55Fe reaction at 16 MeV was performed using the Florida State University Super-Enge Split-Pole Spectrograph to determine single-neutron energies for the…L. A. Riley, I. C. S. Hay, L. T. Baby et al.·Dec 8, 2022SaveLearn
α-cluster decay from 24Mg resonances produced in 12C(16O,24Mg)α reactionA transfer reaction and cluster-decay experiment, 12C(16O,24Mg→α+20Ne)α, was performed at a beam energy of 96 MeV. Both recoil and decay α…Dong-Xi Wang, Yan-Lin Ye, Cheng-Jian Lin et al.·Dec 8, 2022SaveLearn
Search for the Chiral Magnetic Wave in Pb--Pb collisions using the ALICE detectorThe interplay of the chiral anomaly and the strong magnetic field ( 1015 T) created in heavy-ion collisions could give rise to a collective excitation in the quark--gluon plasma called the…Wenya Wu·Dec 8, 2022SaveLearn
Transfer Reactions in Nuclear AstrophysicsTransfer reactions are an important tool in nuclear astrophysics. These reactions allow us to identify states in nuclei and to find the corresponding energies, to determine if these states can…Philip Adsley·Dec 7, 2022SaveLearn
Understanding globular cluster abundances through nuclear reactionsGlobular clusters contain multiple stellar populations, with some previous generation of stars polluting the current stars with heavier elements. Understanding the history of globular clusters is…P Adsley, M Williams, D S Harrouz et al.·Dec 7, 2022SaveLearn
Precision pulse shape simulation for proton detection at the Nab experimentThe Nab experiment at Oak Ridge National Laboratory, USA, aims to measure the beta-antineutrino angular correlation following neutron β decay to an anticipated precision of approximately 0.1\%.…Leendert Hayen, Jin Ha Choi, Dustin Combs et al.·Dec 7, 2022SaveLearn
In-situ measurement of the velocity spectrum of ultracold neutrons and its evolution using an oscillating detectorUltracold neutrons (UCNs) are used in experiments investigating fundamental interactions, testing the Standard Model of particle physics and searching for phenomena beyond it. Knowledge of the energy…D. Rozpedzik, K. Bodek, K. Kirch et al.·Dec 4, 2022SaveLearn
Measurement of the 159Tb(n, γ) cross section at the CSNS Back-n facilityThe stellar (n, γ) cross section data for the mass numbers around A ≈ 160 are of key importance to nucleosynthesis in the main component of the slow neutron capture process, which…S. Zhang, G. Li, W. Jiang et al.·Dec 4, 2022SaveLearn
Measurements of azimuthal anisotropy of nonprompt D0 mesons in PbPb collisions at sNN = 5.02 TeVMeasurements of the elliptic (v2) and triangular (v3) azimuthal anisotropy coefficients are presented for D0 mesons produced in b hadron decays (nonprompt D0 mesons) in lead-lead…CMS Collaboration·Dec 3, 2022SaveLearn
Experimental overview of electromagnetic probes in ultra-relativistic nucleus-nucleus collisionsElectromagnetic probes are not affected by hadronization and provide direct information about the space-time evolution of high-energy nucleus-nucleus collisions. In particular, the measurement of…Klaus Reygers·Dec 2, 2022SaveLearn
Search for ultralight axion dark matter in a side-band analysis of a 199Hg free-spin precession signalUltra-low-mass axions are a viable dark matter candidate and may form a coherently oscillating classical field. Nuclear spins in experiments on Earth might couple to this oscillating axion…C. Abel, N. J. Ayres, G. Ban et al.·Dec 2, 2022SaveLearn
A Strong-QCD Regime Measurement of the Proton's Spin StructureThe theory of the strong force, Quantum Chromodynamics (QCD) remains one of the most important ways to understand the fundamental properties of ordinary matter. However, at low momentum transfer Q2,…David Ruth·Dec 1, 2022SaveLearn
Hot and Cold QCD White Paper from ALICE-USA: Input for 2023 U.S. Long Range Plan for Nuclear ScienceThe ALICE-USA collaboration presents its plans for the 2023 U.S. Long Range Plan for Nuclear Science.N. Alizadehvandchali, N. Apadula, M. Arslandok et al.·Dec 1, 2022SaveLearn
Isoscalar giant monopole strength in 58Ni, 90Zr, 120Sn and 208PbInelastic α-particle scattering at energies of a few hundred MeV and very-forward scattering angles including 0 has been established as a tool for the study of the isoscalar giant…A. Bahini, R. Neveling, P. von Neumann-Cosel et al.·Dec 1, 2022SaveLearn
Secondary Neutron Production from Thick Target Deuteron BreakupThick target deuteron breakup is a variable-energy accelerator-based source of high-energy neutrons, with applications in fundamental and applied nuclear science and engineering. However, the breakup…Jonathan T. Morrell, Andrew S. Voyles, Jon C. Batchelder et al.·Dec 1, 2022SaveLearn
Observation of Directed Flow of Hypernuclei 3H and 4H in s NN = 3 GeV Au+Au Collisions at RHICWe report here the first observation of directed flow (v1) of the hypernuclei 3H and 4H in mid-central Au+Au collisions at s NN = 3 GeV at RHIC. These data…STAR Collaboration, B. E. Aboona, J. Adam et al.·Nov 30, 2022SaveLearn
Dissipative reactions with intermediate-energy beams -- a novel approach to populate complex-structure states in rare isotopesA novel pathway for the formation of multi-particle-multi-hole (np-mh) excited states in rare isotopes is reported from highly energy- and momentum-dissipative inelastic-scattering events measured in…A. Gade, B. A. Brown, D. Weisshaar et al.·Nov 30, 2022SaveLearn
Stellar s-process neutron capture cross sections of 69,71GaThe stable gallium isotopes, 69,71Ga, are mostly produced by the weak slow (s) process in massive stars. We report here on measurements of astrophysically-relevant neutron capture cross…M. Tessler, M. Paul, S. Halfon et al.·Nov 30, 2022SaveLearn
Vector meson photoproduction in UPCs with FoCalWe discuss the physics prospects of photon-induced measurements using the high-granularity FoCal detector to be installed at the ALICE experiment, covering the pseudorapidity interval $3.4 ≤ η…Alexander Bylinkin, Joakim Nystrand, Daniel Tapia Takaki·Nov 29, 2022SaveLearn
Precision Studies of QCD in the Low Energy Domain of the EICThe manuscript focuses on the high impact science of the EIC with objective to identify a portion of the science program for QCD precision studies that requires or greatly benefits from high…V. Burkert, L. Elouadrhiri, A. Afanasev et al.·Nov 28, 2022SaveLearn
Pseudorapidity densities of charged particles with transverse momentum thresholds in pp collisions at s = 5.02 and 13 TeVThe pseudorapidity density of charged particles with minimum transverse momentum (p T) thresholds of 0.15, 0.5, 1, and 2 GeV/c is measured in pp collisions at the centre of mass energies of…ALICE Collaboration·Nov 28, 2022SaveLearn
Multiplicity dependence of charged-particle production in pp, p-Pb, Xe-Xe and Pb-Pb collisions at the LHCMultiplicity (N ch) distributions and transverse momentum (p T) spectra of inclusive primary charged particles in the kinematic range of |η| < 0.8 and 0.15 GeV/c < pT < 10…ALICE Collaboration·Nov 28, 2022SaveLearn