Femtoscopic Proton-Lambda Correlations in Pb-Pb Collisions at sqrt(sNN) = 2.76 TeV with ALICETwo-particle correlations at small relative momenta give insight into the size of the emitting source. Of particular interest is the test of hydrodynamic models which predict a universal, apparent…Hans Beck·Feb 3, 2015SaveLearn
Study of in-medium mass modification at J-PARCStudy of in-medium mass modification has attracted interest in terms of the restoration of the spontaneously broken chiral symmetry, which is responsible for the generation of hadron mass. Many…Kazuya Aoki·Feb 3, 2015SaveLearn
Two-pion femtoscopy in p-Pb collisions at s NN=5.02 TeVWe report the results of the femtoscopic analysis of pairs of identical pions measured in p-Pb collisions at sNN=5.02 TeV. Femtoscopic radii are determined as a function of event…ALICE Collaboration·Feb 2, 2015SaveLearn
Luminosity determination for the deutron-deutron reactions using free and quasi-free reactions with WASA-at-COSY detectorTwo methods of the luminosity determination for the experiment performed by WASA collaboration to search for 4 -0.03cmHe-η bound state are presented. During the measurement the…M. Skurzok, P. Moskal, W. Krzemien·Feb 2, 2015SaveLearn
Event-by-event mean pT fluctuations in pp and Pb-Pb collisions at the LHCThe ALICE detector at the LHC is used to study the properties of the Quark-Gluon Plasma produced in heavy-ion collisions. As a reference measurement, also the analysis of proton-proton (pp)…S. T. Heckel·Feb 2, 2015SaveLearn
Forward-backward multiplicity correlations in pp collisions at s=0.9, 2.76 and 7 TeVThe strength of forward-backward (FB) multiplicity correlations is measured by the ALICE detector in proton-proton (pp) collisions at s=0.9, 2.76 and 7 TeV. The measurement is performed in…ALICE Collaboration·Feb 1, 2015SaveLearn
Evaluation of Stopping Powers of Superheavy Ions with Z up to 124 in Al and UElectronic and nuclear stopping powers of superheavy ions with Z up to 124 and A=300 in Al and U were estimated in the energy range of 0.01-0.20 MeV/u. The corresponding stopping powers…Yong Hee Chung·Feb 1, 2015SaveLearn
Direct probes of neutrino massThe discovery of neutrino oscillations has shown that neutrinos, in contradiction to a prediction of the minimal standard model, have mass. Oscillations do not yield a value for the mass, but do set…R. G. Hamish Robertson·Jan 31, 2015SaveLearn
Precise measurement of the 222Rn half-life: a probe to monitor the stability of radioactivityWe give the results of a study on the 222Rn decay we performed in the Gran Sasso Laboratory (LNGS) by detecting the gamma rays from the radon progeny. The motivation was to monitor the stability of…E. Bellotti, C. Broggini, G. Di Carlo et al.·Jan 30, 2015SaveLearn
High Spin Spectroscopy and Shape Evolution in 105CdHigh spin states in 105Cd were studied using 16O beam on 92Mo reaction at an incident beam energy of 75 MeV. The level scheme of 105Cd has been observed up to an excitation energy of 10.8 MeV with…M. Kumar Raju, D. Negi, S. Muralithar et al.·Jan 30, 2015SaveLearn
Azimuthal Anisotropy Relative to the Participant Plane from AMPT in Central p+Au, d+Au, and 3He+Au Collisions at sNN=200 GeVRecent data from p+p and p+Pb collisions at the Large Hadron Collider (LHC), and d+Au and 3He+Au collisions at the Relativistic Heavy Ion Collider (RHIC) reveal patterns that---when observed in…J. D. Orjuela Koop, A. Adare, D. McGlinchey et al.·Jan 27, 2015SaveLearn
Observation of Lambda H-4 hyperhydrogen by decay-pion spectroscopy in electron scatteringAt the Mainz Microtron MAMI, the first high-resolution pion spectroscopy from decays of strange systems was performed by electron scattering off a Be-9 target in order to study the ground-state…A. Esser, S. Nagao, F. Schulz et al.·Jan 27, 2015SaveLearn
Bubble Chambers for Experiments in Nuclear AstrophysicsA bubble chamber has been developed to be used as an active target system for low energy nuclear astrophysics experiments. Adopting ideas from dark matter detection with superheated liquids, a…B. DiGiovine, D. Henderson, R. J. Holt et al.·Jan 27, 2015SaveLearn
Event geometrical anisotropy and fluctuation viewed by HBT interferometryAzimuthal angle dependence of the pion source radii was measured applying the event shape selection at the PHENIX experiment. The measured final source eccentricity is found to be enhanced when…Takafumi Niida·Jan 27, 2015SaveLearn
2014 Update of the Discoveries of NuclidesThe 2014 update of the discovery of nuclide project is presented. Only six new nuclides were observed for the first time in 2014 while the assignments of seventeen other nuclides were revised. In…M. Thoennessen·Jan 27, 2015SaveLearn
Measurement of heavy-flavour production as a function of multiplicity in pp and p-Pb collisions with ALICEIn these proceedings results are presented from the measurement of open heavy-flavour production as a function of charged-particle multiplicity in pp collisions at s = 7 TeV and p-Pb…Riccardo Russo·Jan 26, 2015SaveLearn
An Upgrade Proposal from the PHENIX CollaborationIn this document the PHENIX collaboration proposes a major upgrade to the PHENIX detector at the Relativistic Heavy Ion Collider. This upgrade, sPHENIX, enables an extremely rich jet and beauty…A. Adare, S. Afanasiev, C. Aidala et al.·Jan 25, 2015SaveLearn
Unprecedented studies of the low-energy negatively charged kaons interactions in nuclear matter by AMADEUSThe AMADEUS experiment aims to provide unique quality data of K- hadronic interactions in light nuclear targets, in order to solve fundamental open questions in the non-perturbative strangeness…C. Curceanu, K. Piscicchia, M. Bazzi et al.·Jan 23, 2015SaveLearn
A precision measurement of the p(e,e p\,)π0 reaction at thresholdNew results are reported from a measurement of π0 electroproduction near threshold using the p(e,e p)π0 reaction. The experiment was designed to determine precisely the energy…K. Chirapatpimol, M. H. Shabestari, R. A. Lindgren et al.·Jan 22, 2015SaveLearn
Modern Studies of the Deuteron: from the Lab Frame to the Light FrontWe review the recent progress made in studies of deuteron structure at small internucleon distances. This progress is largely facilitated by the new generation of experiments in deuteron…Werner Boeglin, Misak Sargsian·Jan 22, 2015SaveLearn
Measurement of the strong interaction induced shift and width of the 1s state of kaonic deuterium at J-PARCThe antikaon-nucleon interaction close to threshold provides crucial information on the interplay between spontaneous and explicit chiral symmetry breaking in low-energy QCD. In this context the…J. Zmeskal, M. Sato, S. Ajimura et al.·Jan 22, 2015SaveLearn
Constraining the nuclear matter equation of state around twice saturation densityUsing FOPI data on elliptic flow in Au+Au collisions between 0.4 and 1.5A GeV we extract constraints for the equation of state (EOS) of compressed symmetric nuclear matter using the transport code…A. Le Fèvre, Y. Leifels, W. Reisdorf et al.·Jan 21, 2015SaveLearn
Average and recommended half-life values for two neutrino double beta decayAll existing positive results on two neutrino double beta decay in different nuclei were analyzed. Using the procedure recommended by the Particle Data Group, weighted average values for half-lives…A. S. Barabash·Jan 21, 2015SaveLearn
Transverse Wobbling in 135PrA pair of transverse wobbling bands has been observed in the nucleus 135Pr. The wobbling is characterized by ΔI =1, E2 transitions between the bands, and a decrease in the wobbling energy…J. T. Matta, U. Garg, W. Li et al.·Jan 21, 2015SaveLearn
Gamma-spectrometric determination of 232U in uranium-bearing materialsThe 232U content of various uranium-bearing items was measured using low-background gamma spectrometry. The method is independent of the measurement geometry, sample form and chemical composition.…Jozsef Zsigrai, Tam Cong Nguyen, Andrey Berlizov·Jan 19, 2015SaveLearn