Anisotropy results from 193 GeV U+U collisions at RHICWe report the measurement of azimuthal anisotropy vn for n = 1-5 as a function of transverse momentum pT and centrality in U+U collisions at sNN = 193 GeV, recorded with the…Yadav Pandit·May 21, 2014SaveLearn
Study of Υ production and cold nuclear matter effects in pPb collisions at sNN=5~TeVProduction of Υ mesons in proton-lead collisions at a nucleon-nucleon centre-of-mass energy sNN=5 TeV is studied with the LHCb detector. The analysis is based on a data sample…LHCb collaboration, R. Aaij, B. Adeva et al.·May 20, 2014SaveLearn
Compton Scattering from 6Li at 86 MeVCross sections for 6Li(γ,γ)6Li have been measured at the High Intensity Gamma-Ray Source () and the sensitivity of these cross sections to the nucleon isoscalar…L. S. Myers, M. W. Ahmed, G. Feldman et al.·May 20, 2014SaveLearn
Polynomial fits and the proton radius puzzleThe Proton Radius Puzzle refers to the ~7σ discrepancy that exists between the proton charge radius determined from muonic hydrogen and that determined from electronic hydrogen spectroscopy and…E. Kraus, K. E. Mesick, A. White et al.·May 19, 2014SaveLearn
Elliptic flow of identified hadrons in Pb-Pb collisions at sNN = 2.76 TeVThe elliptic flow coefficient (v2) of identified particles in Pb-Pb collisions at sNN = 2.76 TeV was measured with the ALICE detector at the LHC. The results were obtained…ALICE Collaboration·May 19, 2014SaveLearn
Neutrinoless double-beta decay of 76Ge and 130Te. A correction of the neutrinoless 2eta-decay model and a reanalysis of QUORICINO resultsA correction of the neutrinoless 2eta-decay model was proposed which predicted a shift of the 2eta0ν-signal from the Q value (2eta-decay energy). The shifts were calculated for 76Ge…I. V. Kirpichnikov·May 19, 2014SaveLearn
A Centrality Detector ConceptThe nucleus-nucleus impact parameter and collision geometry of a heavy ion collision are typically characterized by assigning a collision "centrality". In all present heavy ion experiments…Sourav Tarafdar, Zvi Citron, Alexander Milov·May 18, 2014SaveLearn
Suppression of Υ(1S) at forward rapidity in Pb-Pb collisions at s NN = 2.76 TeVWe report on the measurement of the inclusive Υ(1S) production in Pb-Pb collisions at s NN=2.76 TeV carried out at forward rapidity (2.5<y<4) and down to zero transverse momentum…ALICE Collaboration·May 18, 2014SaveLearn
Beauty production in pp collisions at s = 2.76 TeV measured via semi-electronic decaysThe ALICE collaboration at the LHC reports measurement of the inclusive production cross section of electrons from semi-leptonic decays of beauty hadrons with rapidity |y|<0.8 and transverse…ALICE Collaboration·May 16, 2014SaveLearn
Measurement of electrons from semileptonic heavy-flavor hadron decays in pp collisions at s = 2.76 TeVThe p T-differential production cross section of electrons from semileptonic decays of heavy-flavor hadrons has been measured at mid-rapidity in proton-proton collisions at s = 2.76…ALICE Collaboration·May 16, 2014SaveLearn
The detection of back-to-back proton pairs in Charged-Current neutrino interactions with the ArgoNeuT detector in the NuMI low energy beam lineShort range nucleon-nucleon correlations in nuclei (NN SRC) carry important information on nuclear structure and dynamics. NN SRC have been extensively probed through two-nucleon knock- out reactions…R. Acciarri, C. Adams, J. Asaadi et al.·May 16, 2014SaveLearn
Centrality dependence of low-momentum direct-photon production in Au+Au collisions at s_NN=200 GeVThe PHENIX experiment at RHIC has measured the centrality dependence of the direct photon yield from Au+Au collisions at s_NN=200 GeV down to pT=0.4 GeV/c. Photons are detected…A. Adare, S. Afanasiev, C. Aidala et al.·May 15, 2014SaveLearn
Overview of quarkonia and heavy flavour measurements by CMSThis writeup summarizes recent CMS results on quarkonia measurements in pp, pPb and PbPb collisions at LHC. The excellent muon detection capability of CMS allows measurement of charmonia states at…P. Shukla, CMS collaboration·May 15, 2014SaveLearn
Suppression of ψ(2S) production in p-Pb collisions at s NN = 5.02 TeVThe ALICE Collaboration has studied the inclusive production of the charmonium state ψ(2S) in proton-lead (p-Pb) collisions at the nucleon-nucleon centre of mass energy sNN = 5.02 TeV…ALICE Collaboration·May 15, 2014SaveLearn
Neutral pion production at midrapidity in pp and Pb-Pb collisions at s NN = 2.76 TeVInvariant yields of neutral pions at midrapidity in the transverse momentum range 0.6 < pT < 12 GeV/c measured in Pb-Pb collisions at s NN = 2.76 TeV are presented for six…ALICE Collaboration·May 15, 2014SaveLearn
Cross section for bb production via dielectrons in d+Au collisions at s_NN=200 GeVWe report a measurement of e+e- pairs from semileptonic heavy-flavor decays in d+Au collisions at s_NN=200 GeV. Exploring the mass and transverse-momentum dependence of the…A. Adare, C. Aidala, N. N. Ajitanand et al.·May 15, 2014SaveLearn
NEUT Pion Final State InteractionsThe pion final state interaction model in NEUT is described. Modifications and tuning of the model are validated against neutrino and non-neutrino (pion scattering and photoproduction) data. A method…Patrick de Perio·May 15, 2014SaveLearn
Re-publication of the data from the BILL magnetic spectrometer: The cumulative β spectra of the fission products of 235U, 239Pu, and 241PuIn the 1980s, measurements of the cumulative β spectra of the fission products following the thermal neutron induced fission of 235U, 239Pu, and 241Pu were performed at the magnetic…N. Haag, W. Gelletly, F. von Feilitzsch et al.·May 14, 2014SaveLearn
Measurement of prompt D-meson production in p-Pb collisions at s NN = 5.02 TeVThe p T-differential production cross sections of the prompt charmed mesons D0, D+, D*+ and D s+ and their charge conjugate in the rapidity interval $-0.96 < y cms…ALICE Collaboration·May 14, 2014SaveLearn
Measurement of KS0 and K*0 in p+p, d+Au, and Cu+Cu collisions at s_NN=200 GeVThe PHENIX experiment at the Relativistic Heavy Ion Collider has performed a systematic study of KS0 and K*0 meson production at midrapidity in p+p, d+Au, and Cu+Cu collisions at…A. Adare, S. Afanasiev, C. Aidala et al.·May 14, 2014SaveLearn
Heavy-quark production and elliptic flow in Au+Au collisions at s_NN=62.4 GeVWe present measurements of electrons and positrons from the semileptonic decays of heavy-flavor hadrons at midrapidity (|y|< 0.35) in Au+Au collisions at s_NN=62.4 GeV. The data…A. Adare, C. Aidala, N. N. Ajitanand et al.·May 13, 2014SaveLearn
Transverse momentum dependence of inclusive primary charged-particle production in p-Pb collisions at s NN = 5.02 TeVThe transverse momentum (p T) distribution of primary charged particles is measured at midrapidity in minimum-bias p-Pb collisions at sNN=5.02 TeV with the ALICE…ALICE Collaboration·May 12, 2014SaveLearn
Measurement of polarisation observables in K0sΣ+ photoproduction off the protonThe reaction γ\, p → K0S\,Σ+ is studied in the photon energy range from threshold. Linearly polarised photon beams from coherent bremsstrahlung enabled the first measurement of photon…R. Ewald, A. V. Anisovich, B. Bantes et al.·May 12, 2014SaveLearn
Atomic site sensitive processes in low energy ion-dimer collisionsElectron capture processes for low energy Ar9+ ions colliding on Ar2 dimer targets are investigated, focusing attention on charge sharing as a function of molecule orientation and impact parameter. A…W. Iskandar, J. Matsumoto, A. Leredde et al.·May 12, 2014SaveLearn
The gamma-ray spectrometer HORUS and its applications for nuclear astrophysicsA dedicated setup for the in-beam measurement of absolute cross sections of astrophysically relevant charged-particle induced reactions is presented. These, usually very low, cross sections at…L. Netterdon, V. Derya, J. Endres et al.·May 12, 2014SaveLearn