Photoproduction prospects at the EICWe discuss how photoproduction and electroproduction processes will provide a precise tool to study nuclear structure in the small-x region in the future Electron-Ion Collider. In particular, we…Heikki Mäntysaari·Aug 18, 2017SaveLearn
Nuclear Structure Functions at a Future Electron-Ion ColliderThe quantitative knowledge of heavy nuclei's partonic structure is currently limited to rather large values of momentum fraction x -- robust experimental constraints below x 10-2 at…E. C. Aschenauer, S. Fazio, M. A. C. Lamont et al.·Aug 18, 2017SaveLearn
Nuclear modification factor of D0 mesons in PbPb collisions at sNN = 5.02 TeVThe transverse momentum (pt) spectrum of prompt D0 mesons and their antiparticles has been measured via the hadronic decay channels D0 K- π+ and…CMS Collaboration·Aug 16, 2017SaveLearn
Comment on arXiv:1612.01502 'Is the Trineutron Resonance Lower in Energy than a Tetraneutron Resonance ?'Comment on the article by S. Gandolfi et al. Phys.Rev.Letters 118 (2017), 232501; arXiv:1612.01502 [nucl-th]P. Truöl, J. P. MIller·Aug 15, 2017SaveLearn
Measurement of prompt D0 meson azimuthal anisotropy in PbPb collisions at sNN = 5.02 TeVThe prompt D0 meson azimuthal anisotropy coefficients, v2 and v3, are measured at midrapidity (|y| < 1.0) in PbPb collisions at a center-of-mass energy sNN = 5.02 TeV…CMS Collaboration·Aug 11, 2017SaveLearn
Pygmy and core polarization dipole modes in 206Pb: connecting nuclear structure to stellar nucleosynthesisA high-resolution study of the electromagnetic response of 206Pb below the neutron separation energy is performed using a (γ,γ') experiment at the HIγS facility. Nuclear…A. P. Tonchev, N. Tsoneva, C. Bhatia et al.·Aug 11, 2017SaveLearn
Rapidity correlations in the RHIC Beam Energy Scan DataA pair-normalized two-particle covariance versus the rapidity of the two particles, called R2, was originally studied in ISR and FNAL data in the 1970's. This variable has recently seen…Sedigheh Jowzaee·Aug 10, 2017SaveLearn
Measurement of the helicity asymmetry E in ωπ+π-π0 photoproductionThe double-polarization observable E was studied for the reaction γp pω using the CEBAF Large Acceptance Spectrometer (CLAS) in Hall B at the Thomas Jefferson National Accelerator Facility and…Z. Akbar, P. Roy, S. Park et al.·Aug 8, 2017SaveLearn
Constraints on the chiral magnetic effect using charge-dependent azimuthal correlations in pPb and PbPb collisions at the LHCCharge-dependent azimuthal correlations of same- and opposite-sign pairs with respect to the second- and third-order event planes have been measured in pPb collisions at sNN = 8.16…CMS Collaboration·Aug 4, 2017SaveLearn
The Electron-Ion Collider: Assessing the Energy Dependence of Key MeasurementsWe provide an assessment of the energy dependence of key measurements within the scope of the machine parameters for a U.S. based Electron-Ion Collider (EIC) outlined in the EIC White Paper. We first…E. C. Aschenauer, S. Fazio, J. H. Lee et al.·Aug 4, 2017SaveLearn
Observation of Coherent Elastic Neutrino-Nucleus ScatteringThe coherent elastic scattering of neutrinos off nuclei has eluded detection for four decades, even though its predicted cross-section is the largest by far of all low-energy neutrino couplings. This…D. Akimov, J. B. Albert, P. An et al.·Aug 3, 2017SaveLearn
Partonic Structure of Light NucleiWe propose to study the partonic structure of 4He by measuring the Beam Spin Asymmetry (BSA) in coherent Deeply Virtual Compton Scattering (DVCS) and the differential cross-section of the Deeply…Whitney Armstrong, John Arrington, Ian Cloet et al.·Aug 2, 2017SaveLearn
Solar Neutrinos as Background to Neutrinoless Double-beta Decay ExperimentsSolar neutrinos interact within double-beta decay () detectors and contribute to backgrounds for \ experiments. Background contributions due to charge-current solar neutrino interactions with…S. R. Elliott, H. Ejiri·Aug 2, 2017SaveLearn
Tagged EMC Measurements on Light NucleiWe propose to measure tagged deep inelastic scattering from light nuclei (deuterium and 4He) by detecting the low energy nuclear spectator recoil (p, 3H and 3He) in addition to the scattered…Whitney Armstrong, John Arrington, Ian Cloet et al.·Aug 2, 2017SaveLearn
Spectator-Tagged Deeply Virtual Compton Scattering on Light NucleiThe three-dimensional picture of quarks and gluons in the proton is set to be revealed through Deeply virtual Compton scattering while a critically important puzzle in the one-dimensional picture…Whitney Armstrong, John Arrington, Ian Cloët et al.·Aug 2, 2017SaveLearn
High-precision QEC-value measurement of the superallowed β+ emitter 22Mg and an evaluation of the A=22 isobaric tripletA direct QEC-value measurement of the superallowed β+ emitter 22Mg was performed using TRIUMF's Ion Trap for Atomic and Nuclear science (TITAN). The direct ground-state to…M. P. Reiter, K. G. Leach, O. M. Drozdowski et al.·Aug 1, 2017SaveLearn
The 12C(n, 2n)11C cross section from threshold to 26.5 MeVThe 12C(n, 2n)11C cross section was measured from just below threshold to 26.5 MeV using the Pelletron accelerator at Ohio University. Monoenergetic neutrons, produced via the…M. Yuly, T. Eckert, G. Hartshaw et al.·Jul 28, 2017SaveLearn
A Review of Elliptic Flow of Light Nuclei in Heavy-Ion Collisions at RHIC and LHC EnergiesWe present a review of the measurements of elliptic flow (v2) of light nuclei (d,d, t, 3 He, and 3 He) from the RHIC and LHC experiments. Light…Md. Rihan Haque, Chitrasen Jena, Bedangadas Mohanty·Jul 28, 2017SaveLearn
Proton and neutron electromagnetic form factors and uncertaintiesWe determine the nucleon electromagnetic form factors and their uncertainties from world electron scattering data. The analysis incorporates two-photon exchange corrections, constraints on the low-Q2…Zhihong Ye, John Arrington, Richard J. Hill et al.·Jul 27, 2017SaveLearn
Polarization Transfer Observables in Elastic Electron Proton Scattering at Q2 = 2.5, 5.2, 6.8, and 8.5 GeV2The GEp-III and GEp-2γ experiments were carried out in Jefferson Lab's (JLab's) Hall C from 2007-2008, to extend the knowledge of GEp/GMp to the highest practically achievable Q2…A. J. R. Puckett, E. J. Brash, M. K. Jones et al.·Jul 26, 2017SaveLearn
Muon capture reaction on 100Mo to study nuclear responses for double beta decays and astro-neutrinosThe negative-muon capture reaction (MCR) on the enriched 100Mo isotope was studied for the first time to investigate neutrino nuclear response for neutrino-less double beta decays and supernova…I. H. Hashim, H. Ejiri, T. Shima et al.·Jul 26, 2017SaveLearn
Evaluation of fusion-evaporation cross-section calculationsCalculated fusion-evaporation cross sections from five different codes are compared to experimental data. The present comparison extents over a large range of nuclei and isotopic chains to…B. Blank, G. Canchel, F. Seis et al.·Jul 26, 2017SaveLearn
LUNA: Status and ProspectsThe essential ingredients of nuclear astrophysics are the thermonuclear reactions which shape the life and death of stars and which are responsible for the synthesis of the chemical elements in the…C. Broggini, D. Bemmerer, A. Caciolli et al.·Jul 25, 2017SaveLearn
Effective proton-neutron interaction near the drip line from unbound states in 25,26FBackground: Odd-odd nuclei, around doubly closed shells, have been extensively used to study proton-neutron interactions. However, the evolution of these interactions as a function of the binding…M. Vandebrouck, A. Lepailleur, O. Sorlin et al.·Jul 25, 2017SaveLearn
Technical Supplement to "Polarization Transfer Observables in Elastic Electron-Proton Scattering at Q2 = 2.5, 5.2, 6.8, and 8.5 GeV2"The GEp-III and GEp-2γ experiments, carried out in Jefferson Lab's Hall C from 2007-2008, consisted of measurements of polarization transfer in elastic electron-proton scattering at momentum…A. J. R. Puckett, E. J. Brash, M. K. Jones et al.·Jul 24, 2017SaveLearn