Spectroscopy of the neutron-rich hypernucleus 7ΛHe from electron scatteringThe missing mass spectroscopy of the 7ΛHe hypernucleus was performed, using the 7Li(e,eK+)7ΛHe reaction at the Thomas Jefferson National Accelerator Facility Hall C. The…T. Gogami, C. Chen, D. Kawama et al.·Jun 29, 2016SaveLearn
First Measurement of Collectivity of Coexisting Shapes based on Type II Shell Evolution: The Case of 96ZrBackground: Type II shell evolution has recently been identified as a microscopic cause for nuclear shape coexistence. Purpose: Establish a low-lying rotational band in 96-Zr. Methods:…C. Kremer, S. Aslanidou, S. Bassauer et al.·Jun 29, 2016SaveLearn
Charge-changing-cross-section measurements of 12-16C at around 45A MeV and development of a Glauber model for incident energies 10A-2100A MeVWe have measured for the first time the charge-changing cross sections (σCC) of 12-16C on a 12C target at energies below 100A MeV. To analyze these low-energy data, we have…D. T. Tran, H. J. Ong, T. T. Nguyen et al.·Jun 28, 2016SaveLearn
J/ψ suppression at forward rapidity in Pb-Pb collisions at s NN = 5.02 TeVThe inclusive J/ψ production has been studied in Pn-Pb and pp collisions at the centre-of-mass energy per nucleon pair s NN=5.02 TeV, using the ALICE detector at the CERN LHC. The…ALICE Collaboration·Jun 27, 2016SaveLearn
Three Magnetic Rotation Bands in 84RbHigh-spin states in 84Rb are studied by using the 70Zn(18O, p3n)84Rb reaction at beam energy of 75 MeV. Three high-lying negative-parity bands are established, whose level…Shuifa Shen, Xin Zhao, Guangbing Han et al.·Jun 27, 2016SaveLearn
Finite-Size Scaling of Non-Gaussian Fluctuations Near the QCD Critical PointAn effective Finite-Size Scaling (FSS) of moment products from recent STAR measurements of the variance σ, skewness S and kurtosis κ of net-proton multiplicity distributions, are reported for a…Roy A. Lacey, Peifeng Liu, Niseem Magdy et al.·Jun 26, 2016SaveLearn
Photon asymmetry measurements of γ p → π0 p for Eγ=320-650 MeVHigh statistics measurements of the photon asymmetry Σ for the γp→π0p reaction have been made in the center of mass energy range W=1214-1450 MeV. The data…S. Gardner, D. Howdle, M. H. Sikora et al.·Jun 25, 2016SaveLearn
Enhanced production of multi-strange hadrons in high-multiplicity proton-proton collisionsAt sufficiently high temperature and energy density, nuclear matter undergoes a transition to a phase in which quarks and gluons are not confined: the Quark-Gluon Plasma (QGP) [1]. Such an extreme…ALICE Collaboration·Jun 23, 2016SaveLearn
Beta-delayed gamma decay of 26P: Possible evidence of a proton haloBackground: Measurements of β decay provide important nuclear structure information that can be used to probe isospin asymmetries and inform nuclear astrophysics studies. Purpose: To measure the…D. Pérez-Loureiro, C. Wrede, M. B. Bennett et al.·Jun 21, 2016SaveLearn
Double Beta Decays into Excited States in 110Pd and 102PdA search for double beta decays of 110Pd and 102Pd into excited states of the daughter nuclides has been performed using three ultra-low background gamma-spectrometry measurements in the…B. Lehnert, E. Andreotti, D. Degering et al.·Jun 21, 2016SaveLearn
Evidence for collectivity in pp collisions at the LHCMeasurements of two- and multi-particle angular correlations in pp collisions at sqrt(s) = 5, 7, and 13 TeV are presented as a function of charged-particle multiplicity. The data, corresponding to…CMS Collaboration·Jun 20, 2016SaveLearn
Higher harmonic flow coefficients of identified hadrons in Pb-Pb collisions at s NN = 2.76 TeVThe elliptic, triangular, quadrangular and pentagonal anisotropic flow coefficients for π, K and p+p in Pb-Pb collisions at $sNN =…ALICE Collaboration·Jun 20, 2016SaveLearn
Impact of residual contamination on inclusive and direct photon flowDirect photon flow is measured by subtracting the contribution of decay photon flow from the measured inclusive photon flow via the double ratio R γ, which defines the excess of direct over…F. Bock, C. Loizides, T. Peitzmann et al.·Jun 20, 2016SaveLearn
Improved limit on the 225Ra electric dipole momentBackground: Octupole-deformed nuclei, such as that of 225Ra, are expected to amplify observable atomic electric dipole moments (EDMs) that arise from time-reversal and parity-violating…Michael Bishof, Richard H. Parker, Kevin G. Bailey et al.·Jun 15, 2016SaveLearn
Production of deuterium, tritium, and 3He in central Pb+Pb collisions at 20A, 30A, 40A, 80A, and 158A GeV at the CERN SPSProduction of d, t, and 3He nuclei in central Pb+Pb interactions was studied at five collision energies (sNN= 6.3, 7.6, 8.8, 12.3, and 17.3 GeV) with the NA49 detector at the CERN…NA49 Collaboration, T. Anticic, B. Baatar et al.·Jun 14, 2016SaveLearn
Change of nuclear configurations in the neutrinoless double-β decay of 130Te → 130Xe and 136Xe → 136BaThe change in the configuration of valence protons between the initial and final states in the neutrinoless double-β decay of 130Te → 130Xe and of 136Xe →…J. P. Entwisle, B. P. Kay, A. Tamii et al.·Jun 13, 2016SaveLearn
Open heavy-flavour and quarkonium production in Pb-Pb and p-Pb collisions measured by the ALICE detector at the LHCOpen heavy-flavour and quarkonia measurements are important tools to study the hot and dense partonic medium formed in ultra-relativistic heavy-ion collisions. The modification of their production in…Davide Caffarri·Jun 13, 2016SaveLearn
Cumulants of Net-Proton, Net-Kaon and Net-Charge Multiplicity Distributions in Au+Au Collisions at RHIC BES Energies from UrQMD ModelFluctuations of conserved quantities are sensitive observables to probe the signature of QCD phase transition and critical point in heavy-ion collisions. With the UrQMD model, we have studied the…Ji Xu, Shili Yu, Feng Liu et al.·Jun 13, 2016SaveLearn
Search for an Isospin I =3 DibaryonVarious theoretical calculations based on QCD or hadronic interactions predict that in addition to the recently observed dibaryon resonance d*(2380) with I(JP) = 0(3+) there should also exist…P. Adlarson, W. Augustyniak, W. Bardan et al.·Jun 9, 2016SaveLearn
The structure effects in polarization and cross section in inelastic A(p,p')X reaction with the 40Ca and 12C nuclei at 1 GeVThe polarization of the secondary protons in inelastic (p,p') reaction on the 40Ca and 12C nuclei at the initial proton energy 1 GeV was measured in the wide range of the scattered proton momenta…O. V. Miklukho, A. Yu. Kisselev, G. M. Amalsky et al.·Jun 9, 2016SaveLearn
Anisotropic flow of Pb+Pb s NN = 5.02 TeV from A Multi-Phase Transport ModelAnisotropic flow is an important observable in the study of the Quark-Gluon Plasma that is expected to be formed in heavy-ion collisions. With a multiphase transport (AMPT) model we investigate the…Zhao Feng, Guang-Ming Huang, Feng Liu·Jun 8, 2016SaveLearn
Ultra-Peripheral Collisions with gold ions in STARIn 2010, the STAR Collaboration collected 38 million low-multiplicity triggers for ultra-peripheral collision studies. We present new results involving photonuclear interactions in ultra-peripheral…Spencer R. Klein·Jun 8, 2016SaveLearn
Measurements of the Separated Longitudinal Structure Function FL from Hydrogen and Deuterium Targets at Low Q2Structure functions, as measured in lepton-nucleon scattering, have proven to be very useful in studying the quark dynamics within the nucleon. However, it is experimentally difficult to separately…V. Tvaskis, A. Tvaskis, I. Niculescu et al.·Jun 8, 2016SaveLearn
Optical model potential of deuteron with 1p-shell nucleiA set of global optical potential parameters, DA1p, for deuterons with the 1p-shell nuclei is obtained by simultaneously fitting 67 sets of experimental data of deuteron elastic scattering from…Y. Zhang, D. Y. Pang, J. L. Lou·Jun 5, 2016SaveLearn
Measurement of the p(e,e'π+)n reaction close to threshold and at low Q2The cross section of the p(e,e'π+)n reaction has been measured for five kinematic settings at an invariant mass of W = 1094 MeV and for a four-momentum transfer of Q2 = 0.078…A1 Collaboration, I. Friščić, P. Achenbach et al.·Jun 3, 2016SaveLearn