Experimentally constrained (p,γ)89Y and (n,γ)89Y reaction rates relevant to the p-process nucleosynthesisThe nuclear level density and the γ-ray strength function have been extracted for 89Y, using the Oslo Method on 89Y(p,p' γ)89Y coincidence data. The γ-ray strength function…A. C. Larsen, M. Guttormsen, R. Schwengner et al.·Oct 4, 2015SaveLearn
To the measurement of the radius via an electron scatteringWe propose an experiment for an accurate measurement of the proton radius. A key feature of our proposal is an iron-free magnetic spectrometer. Projected systematics uncertainties will allow a 1%…B. Wojtsekhowski·Oct 4, 2015SaveLearn
Energy scan of correlations in p+p and Be+Be from NA61/SHINEThe existence of the critical point (CP) of strongly interacting matter is still an open problem. An extensive strong interactions program including a search of the CP and the study of the onset of…Andrey Seryakov·Oct 3, 2015SaveLearn
Measurement of D-meson production in Pb-Pb collisions at the LHC with ALICEThe measurement of D-meson production in heavy-ion collisions at LHC energy provides insights into the mechanisms of interaction of charm quarks in the hot and dense medium formed in these…Andrea Festanti·Oct 3, 2015SaveLearn
3D Structure and Nuclear TargetsRecent experimental and theoretical ideas are laying the ground for a new era in the knowledge of the parton structure of nuclei. We report on two promising directions beyond inclusive deep inelastic…R. Dupré, S. Scopetta·Oct 3, 2015SaveLearn
Search for two-neutrino double electron capture on 124Xe with the XMASS-I detectorDouble electron capture is a rare nuclear decay process in which two orbital electrons are captured simultaneously in the same nucleus. Measurement of its two-neutrino mode would provide a new…XMASS Collaboration, K. Abe, K. Hiraide et al.·Oct 2, 2015SaveLearn
Modifications of Nucleons in NucleiI summarize recent results and discuss upcoming and planned experiments that attempt to elucidate how the structure of nucleons might be modified by nuclear binding.Sebastian E. Kuhn·Oct 2, 2015SaveLearn
Energy dependence of hadron spectra and yields in p+p and 7Be+9Be collisions from the NA61/SHINE experiment at the CERN SPSThe NA61/SHINE programme on strong interactions covers the study of the onset of deconfinement and aims to discover the critical point of strongly interacting matter by performing an energy and…D. T. Larsen·Oct 2, 2015SaveLearn
A Future Polarized Drell-Yan Experiment at FermilabOne of the great challenges of QCD is trying to understand the origin of the nucleon spin. Several decades of experimental measurements have shown that our current understanding is incomplete if only…David Kleinjan·Oct 2, 2015SaveLearn
Production of Quarkonia at RHICThe production of different quarkonium states provides unique insight to the hot and cold nuclear matter effects in the strongly interacting medium that is formed in high energy heavy ion collisions.…Robert Vertesi·Oct 2, 2015SaveLearn
Soft photon registration at NuclotronFirst results of a soft photon yield in nucleus-nuclear interactions at 3.5 GeV per nucleon are presented. These photons have been registered at Nuclotron (LHEP, JINR) by an electromagnetic…Elena Kokoulina, E. Ardashev, V. Golovkin et al.·Oct 2, 2015SaveLearn
First Measurement of the Beam Normal Single Spin Asymmetry in Δ Resonance Production by Q weakThe beam normal single spin asymmetry (B n) is generated in the scattering of transversely polarized electrons from unpolarized nuclei. The asymmetry arises from the interference of the…Nuruzzaman·Oct 1, 2015SaveLearn
Collectivity in Small QCD SystemsFeatures of collectivity observed in high energy A+A collision systems at the Relativistic Heavy Ion Collider (RHIC) and the Large Hadron Collider (LHC) imply a strongly coupled quark gluon plasma…Theodore Koblesky·Oct 1, 2015SaveLearn
Energy dependence of fluctuations in p+p and Be+Be collisions from NA61/SHINEThe main aims of the NA61/SHINE experiment are to discover the critical point of strongly interacting matter and to study properties of the onset of deconfinement. For this goal a two dimensional…Evgeny Andronov·Oct 1, 2015SaveLearn
Disentangling random thermal motion of particles and collective expansion of source from transverse momentum spectra in high energy collisionsIn the framework of a multisource thermal model, we describe experimental results of the transverse momentum spectra of final-state light flavour particles produced in gold-gold (Au-Au),…Hua-Rong Wei, Fu-Hu Liu, Roy A. Lacey·Sep 30, 2015SaveLearn
Measurement of transverse momentum relative to dijet systems in PbPb and pp collisions at sqrt(s[NN]) = 2.76 TeVAn analysis of dijet events in PbPb and pp collisions is performed to explore the properties of energy loss by partons traveling in a quark-gluon plasma. Data are collected at a nucleon-nucleon…CMS Collaboration·Sep 30, 2015SaveLearn
Longitudinal Spin Physics at RHIC and a Future eRHICRecent highlights from the spin program at the Relativistic Heavy Ion Collider (RHIC), focusing on the gluon contribution to the proton spin and the polarization of the light flavor sea, are…Brian Page·Sep 30, 2015SaveLearn
The Qweak Experiment: First Determination of the Weak Charge of the ProtonThe Qweak Collaboration has completed a challenging measurement of the parity-violating asymmetry in elastic electron-proton (ep) scattering at the Thomas Jefferson National Accelerator…Manolis Kargiantoulakis·Sep 29, 2015SaveLearn
Measurement of an excess in the yield of J/ψ at very low p T in Pb-Pb collisions at s NN = 2.76 TeVWe report on the first measurement of an excess in the yield of J/ψ at very low transverse momentum (p T< 0.3 GeV/c) in peripheral hadronic Pb-Pb collisions at s NN = 2.76…ALICE Collaboration·Sep 29, 2015SaveLearn
Pseudorapidity and transverse-momentum distributions of charged particles in proton-proton collisions at s = 13 TeVThe pseudorapidity (η) and transverse-momentum (p T) distributions of charged particles produced in proton-proton collisions are measured at the centre-of-mass energy s = 13 TeV.…ALICE Collaboration·Sep 29, 2015SaveLearn
Di-Jet Imbalance Measurements in Central Au+Au Collisions at sNN=200 GeV from STARThe STAR collaboration reports the first measurements of the transverse momentum asymmetry AJ of di-jet pairs in central gold-gold collisions and minimum bias proton-proton collisions at…Kolja Kauder·Sep 29, 2015SaveLearn
On pseudorapidity distribution and speed of sound in high energy heavy ion collisions based on a new revised Landau hydrodynamic modelWe propose a new revised Landau hydrodynamic model to study systematically the pseudorapidity distributions of charged particles produced in heavy ion collisions over an energy range from a few GeV…Li-Na Gao, Fu-Hu Liu·Sep 29, 2015SaveLearn
A study of transverse momentum distributions of jets produced in p-p, p- p, d-Au, Au-Au, and Pb-Pb collisions at high energiesThe transverse momentum distributions of jets produced in p-p, p- p, d-Au, Au-Au, and Pb-Pb collisions at high energies with different selected conditions are analyzed by using a multi-source…Hua-Rong Wei, Fu-Hu Liu·Sep 29, 2015SaveLearn
Centrality dependence of identified particle elliptic flow in relativistic heavy ion collisions at sqrt(s)= 7.7--62.4 GeVElliptic flow (v2) values for identified particles at midrapidity in Au + Au collisions measured by the STAR experiment in the Beam Energy Scan at the Relativistic Heavy Ion Collider at…STAR Collaboration, L. Adamczyk, J. K. Adkins et al.·Sep 28, 2015SaveLearn
Test of Lorentz Invarience from Compton ScatteringIn the recent times, test of Lorentz Invariance has been used as a means to probe theories of physics beyond the standard model. We describe a simple way of utilizing the polarimeters, which are a…Prajwal Mohanmurthy, Dipangkar Dutta, Amrendra Narayan·Sep 28, 2015SaveLearn