Nuclear Physics Programs for the Future Rare Isotope Beams Accelerator Facility in KoreaWe present nuclear physics programs based on the planned experiments using rare isotope beams (RIBs) for the future Korean Rare Isotope Beams Accelerator facility; RAON. This ambitious facility has…Chang-Bum Moon·Jan 27, 2016SaveLearn
Upper limits for the production of the eta-mesic Helium in the dd ->3Henpi0 and dd -> 3Heppi- reactionsWe performed a search for 4He-eta bound state in dd -> 3Henpi0 and dd -> 3Heppi- reactions with the WASA-at-COSY facility using a ramped beam technique. The measurement was carried out with high…M. Skurzok, W. Krzemien, O. Rundel et al.·Jan 26, 2016SaveLearn
Structure near K-+p+p threshold in the in-flight 3He(K-,Λp)n reactionTo search for an S= -1 di-baryonic state which decays to Λp, the 3He(K-,Λp)nmissing reaction was studied at 1.0 GeV/c. Unobserved neutrons were kinematically identified from the…PARC E15 Collaboration, Y. Sada, S. Ajimura et al.·Jan 26, 2016SaveLearn
Measuring the Weak Charge of the Proton via Elastic Electron-Proton ScatteringThe Qweak experiment which ran at Jefferson Lab in Newport News, VA, measured the weak charge of the proton QWp via elastic electron-proton scattering. Longitudinally polarized electrons were…Donald Jones·Jan 26, 2016SaveLearn
Measurement of elliptic flow of light nuclei at sNN = 200, 62.4, 39, 27, 19.6, 11.5, and 7.7 GeV at RHICWe present measurements of 2nd order azimuthal anisotropy (v2) at mid-rapidity (|y|<1.0) for light nuclei d, t, 3He (for sNN = 200, 62.4, 39, 27, 19.6, 11.5, and 7.7 GeV)…STAR Collaboration, L. Adamczyk, J. K. Adkins et al.·Jan 26, 2016SaveLearn
Deuteron-deuteron collision at 160 MeVThe experiment was carried out using BINA detector at KVI in Groningen. For the first time an extensive data analysis of the data collected in back part of the detector is presented, where a…G. Khatri, W. Parol, K. Bodek et al.·Jan 25, 2016SaveLearn
Scaling properties of the mean multiplicity and pseudorapidity density in e-+e+, e+p, p(p)+p, p+A and A+A(B) collisionsThe pseudorapidity density (dN/deta) for p+p, p+A and A+A(B) collisions, and the mean multiplicity <Nch> for ee, ep, and p+p collisions, are studied for an inclusive range of beam energies (Roots).…Roy A. Lacey, Peifeng Liu, Niseem Magdy et al.·Jan 22, 2016SaveLearn
N * decays to Nω from new data on γp ωpData on the reaction γp ωp with ωπ0γ, taken with unpolarized or polarized beams in combination with an unpolarized or polarized proton-target, were analyzed within the Bonn-Gatchina (BnGa)…I. Denisenko, A. V. Anisovich, V. Crede et al.·Jan 22, 2016SaveLearn
Specific Heat of Matter Formed in Relativistic Nuclear CollisionsWe report the excitation energy dependence of specific heat () of hadronic matter at freeze-out in Au+Au and Cu+Cu collisions at the Relativistic Heavy Ion Collider energies by analyzing the…Sumit Basu, Sandeep Chatterjee, Rupa Chatterjee et al.·Jan 21, 2016SaveLearn
New limits on double beta processes in 106-CdA radiopure cadmium tungstate crystal scintillator, enriched in 106-Cd to 66%, with mass of 216 g (106-CdWO4) was used in coincidence with four ultra-low background HPGe detectors contained in a…V. I. Tretyak, P. Belli, R. Bernabei et al.·Jan 21, 2016SaveLearn
Femtoscopic measurements in p+Pb collisions at s_NN= 5.02~TeV with ATLAS at the LHCRecent measurements in two-particle correlations in p+Pb collisions suggest collective behavior reminiscent of that observed in Pb+Pb. Femtoscopic measurements may provide useful insight on this…Markus K. Koehler·Jan 21, 2016SaveLearn
Search for double beta decay of 116Cd with enriched 116CdWO4 crystal scintillators (Aurora experiment)The Aurora experiment to investigate double beta decay of 116Cd with the help of 1.162 kg cadmium tungstate crystal scintillators enriched in 116Cd to 82\% is in progress at the Gran Sasso…F. A. Danevich, A. S. Barabash, P. Belli et al.·Jan 21, 2016SaveLearn
Measurement of the np dπ0π0 Reaction with Polarized Beam in the Region of the d*(2380) ResonanceWe report on a high-statistics measurement of the most basic double pionic fusion reaction np dπ0π0 over the energy region of the d*(2380) resonance by use of a polarized deuteron…P. Adlarson, W. Augustyniak, W. Bardan et al.·Jan 20, 2016SaveLearn
LUMINEU: a search for neutrinoless double beta decay based on ZnMoO4 scintillating bolometersThe LUMINEU is designed to investigate the possibility to search for neutrinoless double beta decay in 100Mo by means of a large array of scintillating bolometers based on ZnMoO4 crystals…E. Armengaud, Q. Arnaud, C. Augier et al.·Jan 19, 2016SaveLearn
Estimation of double differential angle-dependent neutron production cross sections from tritons on 197Au at energies from 5.97 to 19.14 MeVEstimated cross sections for neutron production from triton bombardment of gold are deduced from measurements of triton interactions with gas targets that used gold as a triton beam stop material.…Manfred Drosg, Bernard Hoop·Jan 19, 2016SaveLearn
Spectroscopy of 232U in the (p,t) reaction: More information on 0+ statesThe excitation spectra in the deformed nucleus 232U have been studied by means of the (p,t) reaction, using the Q3D spectrograph facility at the Munich Tandem accelerator. The angular distributions…A. I. Levon, P. Alexa, G. Graw et al.·Jan 19, 2016SaveLearn
New activation cross section data on longer lived radio-nuclei produced in proton induced nuclear reaction on zirconiumIn the frame of a systematic study of charged particle production routes of medically relevant radionuclei, the excitation function for indirect production of 178mTa through…F. Tárkányi, F. Ditrói, S. Takács et al.·Jan 19, 2016SaveLearn
Coulomb breakup of neutron-rich 29,30Na isotopes near the island of inversionFirst results are reported on the ground state configurations of the neutron-rich 29,30Na isotopes, obtained via Coulomb dissociation (CD) measurements as a method of the direct probe. The…A . Rahaman, Ushasi Datta, T. Aumann et al.·Jan 15, 2016SaveLearn
Beta decay of the exotic Tz = -2 nuclei 48Fe, 52Ni and 56ZnThe results of a study of the beta decays of three proton-rich nuclei with Tz=-2, namely 48Fe, 52Ni and 56Zn, produced in an experiment carried out at GANIL, are reported. In…S. E. A. Orrigo, B. Rubio, Y. Fujita et al.·Jan 15, 2016SaveLearn
Examination of experimental conditions for the production of proton-rich and neutron-rich hypernucleiAfter the demonstration of the feasibility of hypernuclear spectroscopy with heavy-ion beams, the HypHI Collaboration will next focus on the study of proton- and neutron-rich hypernuclei. The use of…C. Rappold, J. F. López Fidalgo·Jan 15, 2016SaveLearn
Multiplicity dependence of charged pion, kaon, and (anti)proton production at large transverse momentum in p-Pb collisions at s NN = 5.02 TeVThe production of charged pions, kaons and (anti)protons has been measured at mid-rapidity (-0.5 < y < 0) in p-Pb collisions at s NN=5.02 TeV using the ALICE detector at the LHC.…ALICE Collaboration·Jan 14, 2016SaveLearn
Low-energy neutrinosThere exist several kinds of sources emitting neutrinos in the MeV energy range. These low-energy neutrinos from different sources can be often detected by the same multipurpose detectors. The…Livia Ludhova·Jan 14, 2016SaveLearn
An introduction to mesic nucleiThere is much speculation and a modest amount of evidence that certain mesons might form quasi-bound states with nuclei to produce really exotic states of matter. For this to be a practical…Colin Wilkin·Jan 14, 2016SaveLearn
PHENIX results on centrality dependence of yields and correlations in d+Au collisions at s_NN=200\,GeVPHENIX has measured the transverse momentum (p T) spectra and two particle angular correlations for high p T particles in d+Au collisions at s_NN=200\,GeV using the…Takao Sakaguchi·Jan 14, 2016SaveLearn
Competition of β-delayed protons and β-delayed γ rays in 56Zn and the exotic β-delayed γ-proton decayRemarkable results have been published recently on the β decay of 56Zn. In particular, the rare and exotic β-delayed γ-proton emission has been detected for the first time in the fp…S. E. A. Orrigo, B. Rubio, Y. Fujita et al.·Jan 13, 2016SaveLearn