Interaction of 160 GeV- Muon with Emulsion NucleiIn this work we present some results of the interaction of high energy muons with emulsion nuclei. The interaction results in emission of a number of fragments as a consequence of electromagnetic…S. M. Othman, M. T. Ghoneim, M. T. Hussein et al.·Jan 13, 2018SaveLearn
Production of D_S meson in Au+Au collision at sNN = 200 GeVWe present the invariant yield and elliptic flow of D_S as a function of transverse momentum in Au+Au collisions at sNN = 200 GeV. The nuclear modification factors of…Md Nasim·Jan 12, 2018SaveLearn
The Compression-Mode Giant Resonances and Nuclear IncompressibilityThe compression-mode giant resonances, namely the isoscalar giant monopole and isoscalar giant dipole modes, are examples of collective nuclear motion. Their main interest stems from the fact that…Umesh Garg, Gianluca Colò·Jan 11, 2018SaveLearn
N-N, PT-N and PT-PT fluctuations in nucleus-nucleus collisions at the NA61/SHINE experimentThe NA61/SHINE experiment aims to discover the critical point of strongly interacting matter and study the properties of the onset of deconfinement. For these goals a scan of the two dimensional…Evgeny Andronov·Jan 11, 2018SaveLearn
Small System Collectivity in Relativistic Hadron and Nuclear CollisionsThe bulk motion of nuclear matter at the ultra-high temperatures created in heavy-ion collisions at the Relativistic Heavy Ion Collider and the Large Hadron Collider is well described in terms of…J. L. Nagle, W. A. Zajc·Jan 10, 2018SaveLearn
Improved search for two-neutrino double electron capture on 124Xe and 126Xe using particle identification in XMASS-IWe conducted an improved search for the simultaneous capture of two K-shell electrons on the 124Xe and 126Xe nuclei with emission of two neutrinos using 800.0 days of data from the…XMASS Collaboration, K. Abe, K. Hiraide et al.·Jan 10, 2018SaveLearn
PHENIX results on three-particle Bose-Einstein correlations in SNN = 200 GeV Au+Au collisionsBose-Einstein correlations of identical hadrons reveal information about hadron creation from the strongly interacting matter formed in ultrarelativistic heavy ion collisions. The measurement of…Tamás Novák·Jan 10, 2018SaveLearn
Cadmium Resonance Parameters from Neutron Capture and Transmission Measurements at the RPI LINACCadmium has been used historically as an important component of integral experiments because of its high thermal neutron absorption cross section. Correct interpretation of such experiments depends…G. Leinweber, D. P. Barry, R. C. Block et al.·Jan 10, 2018SaveLearn
Lifetimes of low-lying excited states in 8636Kr50The evolution of nuclear magic numbers at extremes of isospin is a topic at the forefront of contemporary nuclear physics. N=50 is a prime example, with increasing experimental data coming to light…J. Henderson, A. Chester, G. C. Ball et al.·Jan 9, 2018SaveLearn
New mass anchor points for neutron-deficient heavy nuclei from direct mass measurements of radium and actinium isotopesThe masses of the exotic isotopes 210-214Ac and 210-214Ra have been measured with a multi-reflection time-of-flight mass spectrograph. These isotopes were obtained in flight as…M. Rosenbusch, Y. Ito, P. Schury et al.·Jan 9, 2018SaveLearn
Probing the single-particle character of rotational states in 19F using a short-lived isomeric beamA beam containing a substantial component of both the Jπ=5+, T1/2=162 ns isomeric state of 18F and its 1+, 109.77-min ground state has been utilized to study members of the…D. Santiago-Gonzalez, K. Auranen, M. L. Avila et al.·Jan 8, 2018SaveLearn
Proton charge radius from electron scatteringThe rms-radius R of the proton charge distribution is a fundamental quantity needed for precision physics. This radius, traditionally determined from elastic electron-proton scattering via the…Ingo Sick·Jan 5, 2018SaveLearn
Chronology of the three-body dissociation of 8HeThe space and time configurations of the dissociation of 8He into 6He+n+n, on C and Pb targets, have been explored simultaneously for the first time. The final-state interactions in the…B. Laurent, F. M. Marqués, C. Angulo et al.·Jan 4, 2018SaveLearn
Components of polarization-transfer to a bound proton in a deuteron measured by quasi-elastic electron scatteringWe report the first measurements of the transverse (Px and Py) and longitudinal (Pz) components of the polarization transfer to a bound proton in the deuteron via the…A1 Collaboration, D. Izraeli, I. Yaron et al.·Jan 4, 2018SaveLearn
Separated Kaon Electroproduction Cross Section and the Kaon Form Factor from 6 GeV JLab DataThe 1H(e,e K+)Λ reaction was studied as a function of the Mandelstam variable -t using data from the E01-004 (FPI-2) and E93-018 experiments that were carried out in Hall C at the…M. Carmignotto, S. Ali, K. Aniol et al.·Jan 4, 2018SaveLearn
Two-particle correlations in azimuthal angle and pseudorapidity in Be+BeThe NA61/SHINE experiment aims to discover the critical point of strongly interacting matter and study the properties of the onset of deconfinement. These goals are to be achieved by performing a two…Bartosz Maksiak·Jan 3, 2018SaveLearn
Fission fragment mass distribution in 210Po and 213AtBackground: The influence of shell effect on the dynamics of the fusion fission process and it's evolution with excitation energy in the pre-actinide Hg-Pb region in general is a matter of…A. Sen, T. K. Ghosh, S. Bhattacharya et al.·Jan 3, 2018SaveLearn
Direct Measurement of Astrophysically Important Resonances in 38K(p, γ)39CaAccording to sensitivity studies, the 38K( p, γ)39Ca reaction has a significant influence on Ar, K, and Ca production in…G. Christian, G. Lotay, C. Ruiz et al.·Jan 2, 2018SaveLearn
Fluctuations and correlations from NA61/SHINEBasic ideas, methods and results related to the NA61/SHINE study of event-by-event fluctuations in high energy nuclear collisions are briefly reviewed.Marek Gazdzicki·Dec 30, 2017SaveLearn
Directed flow in Au+Au collisions from the RHIC Beam Energy Scan at the STAR experimentWe report results of v1(y) and dv1/dy near mid-rapidity for π, K, Ks0, p, p, Λ, Λ and ϕ from Beam Energy Scan Au+Au collisions at…Subhash Singha·Dec 29, 2017SaveLearn
Two-pion and two-kaon femtoscopic correlations in Au+Au collisions at sNN=200 GeV from STARMeasurement of femtoscopic correlations in heavy-ion collisions can provide information about spatial and temporal parameters of the particle emission region at kinetic freeze-out. In this work we…Grigory Nigmatkulov·Dec 28, 2017SaveLearn
Search for Deeply Bound Kaonic Nuclear States with AMADEUSWe briefly report on the search for Deeply Bound Kaonic Nuclear States with AMADEUS in the Sigma0 p channel following K- absorption on 12C and outline future perspectives for this work.M. Skurzok, M. Cargnelli, C. Curceanu et al.·Dec 28, 2017SaveLearn
Λ c+ production in pp collisions at s = 7 TeV and in p-Pb collisions at s NN = 5.02 TeVThe p T-differential production cross section of prompt Λ c+ charmed baryons was measured with the ALICE detector at the Large Hadron Collider (LHC) in pp collisions at $s =…ALICE Collaboration·Dec 27, 2017SaveLearn
Exploring Zeptosecond Quantum Equilibration Dynamics: From Deep-Inelastic to Fusion-Fission Outcomes in 58Ni+60Ni ReactionsEnergy dissipative processes play a key role in how quantum many-body systems dynamically evolve towards equilibrium. In closed quantum systems, such processes are attributed to the transfer of…E. Williams, K. Sekizawa, D. J. Hinde et al.·Dec 26, 2017SaveLearn
Measurement of prompt and nonprompt charmonium suppression in PbPb collisions at 5.02 TeVThe nuclear modification factors of J/ and (2S) mesons are measured in PbPb collisions at a centre-of-mass energy per nucleon pair of sNN = 5.02 TeV. The analysis is…CMS Collaboration·Dec 24, 2017SaveLearn