First measurement of coherent double neutral-pion photoproduction on the deuteron at incident energies below 0.9 GeVThe total cross sections were measured for coherent double neutral-pion photoproduction on the deuteron at incident energies below 0.9 GeV for the first time. No clear resonance-like behavior is…T. Ishikawa, H. Fujimura, H. Fukasawa et al.·Oct 18, 2016SaveLearn
Transverse momentum and multiplicity fluctuations in Ar+Sc collisions at the CERN SPS from NA61/SHINEThe 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·Oct 18, 2016SaveLearn
PHENIX results on Lévy analysis of Bose-Einstein correlation functionsThe nature of the quark-hadron phase transition can be investigated through analyzing the space-time structure of the hadron emission source. For this, the Bose-Einstein or HBT correlations of…Dániel Kincses·Oct 17, 2016SaveLearn
Proton-proton correlations in distinguishing the two-proton emission mechanism of 23Al and 22MgThe proton-proton momentum correlation functions (Cpp(q)) for kinematically complete decay channels of 23Al → p + p + 21Na and 22Mg → p + p + 20Ne…D. Q. Fang, Y. G. Ma, X. Y. Sun et al.·Oct 15, 2016SaveLearn
Thick-target transmission method for excitation functions of interaction cross sectionsWe propose a method, called as thick-target transmission (T3) method, to obtain an excitation function of interaction cross sections. In an ordinal experiment to measure the excitation function of…M. Aikawa, S. Ebata, S. Imai·Oct 15, 2016SaveLearn
A new method for measuring the neutron lifetime using an in situ neutron detectorThe neutron lifetime is important in understanding the production of light nuclei in the first minutes after the big bang and it provides basic information on the charged weak current of the standard…C. L. Morris, E. R. Adamek, L. J. Broussard et al.·Oct 14, 2016SaveLearn
CUORE-0 background analysis and evaluation of 130Te 2νββ decay half-lifeCUORE is a bolometric experiment that will search for the Neutrinoless Double Beta decay of 130Te. CUORE-0 is a single CUORE-like tower that was run between 2013 and 2015 to test the performance…Davide Chiesa·Oct 14, 2016SaveLearn
η bound state: theory and experimentThe search for a quasi bound η meson in atomic nuclei is reviewed. This tentative state is studied theoretically as well as experimentally.Hartmut Machner·Oct 14, 2016SaveLearn
Activation cross sections of proton induced nuclear reactions on gold up to 65 MeVActivation cross sections of proton induced reactions on gold for production of 197m,197g,195m,195g, 193m,193g,192Hg, 196m,196g(cum),195g(cum),194,191(cum)Au, 191(cum)Pt and 192Ir…F. Ditrói, F. Tárkányi, S. Takács et al.·Oct 14, 2016SaveLearn
Experimental Overview of Open Heavy FlavorThese are the proceedings of the experimental overview of the production of open heavy flavor at the international conference Strangeness in Quark Matter 2016. Instead of a comprehensive overview, I…Kai Schweda·Oct 13, 2016SaveLearn
Activation cross-sections of proton induced reactions on vanadium in the 37-65 MeV energy rangeExperimental excitation functions for proton induced reactions on natural vanadium in the 37-65 MeV energy range were measured with the activation method using a stacked foil irradiation technique.…F. Ditrói, F. Tárkányi, S. Takács et al.·Oct 13, 2016SaveLearn
Higher order moments of net-charge and multiplicity distributions in p+p interactions at SPS energies from NA61/SHINENA61/SHINE at the CERN SPS is a fixed-target experiment pursuing a rich physics program including measurements for heavy ion, neutrino and cosmic ray physics. The main goal of the ion program is to…Maja Mackowiak-Pawlowska·Oct 12, 2016SaveLearn
Combined Partial Wave Analysis for the description of exclusive p+p p + K+ + Λ productionThe production of p K+ Λ in elementary p + p collision was investigated using the Bonn Gatchina Partial Wave Analysis framework. This approach allows the determination of possible participating…Robert Muenzer·Oct 12, 2016SaveLearn
Symmetry energy and densityThe nuclear equation-of-state is a topic of highest current interest in nuclear structure and reactions as well as in astrophysics. In particular, the equation-of-state of asymmetric matter and the…Wolfgang Trautmann, Mircea Dan Cozma, Paolo Russotto·Oct 12, 2016SaveLearn
Activation cross sections of deuteron induced reactions on niobium in the 30-50 MeV energy rangeActivation cross-sections of deuterons induced reactions on Nb targets were determined with the aim of different applications and comparison with theoretical models.F. Ditrói, F. Tárkányi, S. Takács et al.·Oct 12, 2016SaveLearn
Measurement of the ratio of the sixth order to the second order cumulant of net-proton multiplicity distributions in relativistic heavy-ion collisionsWe investigate the measurement of the sixth order cumulant and its ratio to the second order cumulant (C6/C2) in relativistic heavy-ion collisions. The influence of statistics and different…Lizhu Chen, Zhiming Li, Fenping Cui et al.·Oct 11, 2016SaveLearn
Multiplicity dependence of light flavour hadron production at LHC energies in the strangeness canonical suppression pictureWe present an analysis of data on light flavour hadron production as function of event multiplicity at LHC energies measured by the ALICE collaboration. The strangeness-canonical approach within the…Vytautas Vislavicius, Alexander Kalweit·Oct 10, 2016SaveLearn
Beta-decay study of Tz=-2 proton-rich nucleus 20MgThe β decay of the drip-line nucleus 20Mg gives important information on resonances in 20Na, which are relevant for the astrophysical rp-process. A detailed β decay spectroscopic…L. J. Sun, X. X. Xu, C. J. Lin et al.·Oct 10, 2016SaveLearn
The PANDA Experiment at FAIR - Subatomic Physics with AntiprotonsThe non-perturbative nature of the strong interaction leads to spectacular phenomena, such as the formation of hadronic matter, color confinement, and the generation of the mass of visible matter. To…Johan Messchendorp·Oct 10, 2016SaveLearn
First measurement of unpolarized SIDIS cross section and cross section ratios from a 3He targetThe unpolarized semi-inclusive deep-inelastic scattering (SIDIS) differential cross sections in 3He(e,eπ)X have been measured for the first time in Jefferson Lab experiment…X. Yan, K. Allada, K. Aniol et al.·Oct 7, 2016SaveLearn
Small x gluon shadowing from LHC data on coherent J/ψ photoproductionThe cross section for coherent J/ψ photoproduction in Pb-Pb collisions is the sum of two contributions, one from low-, the other from high-energy photon-nucleus interactions. A novel…J. G. Contreras·Oct 7, 2016SaveLearn
Measurement of the ω π+ π- π0 Dalitz plot distributionUsing the production reactions pd 3He\,ω and pp ppω, the Dalitz plot distribution for the ω π+ π- π0 decay is studied with the WASA detector at COSY, based on a combined…COSY Collaboration, P. Adlarson, W. Augustyniak et al.·Oct 7, 2016SaveLearn
K-K-pp - an important gateway toward multi-kaonic nucleiBased on our Faddeev-Yakubowsky calculations of four-body kaonic nuclear systems it was revealed that the structure of K-K-pp is well approximated by two Lambda*=K-p's with strong mutual…Shuji Maeda, Yoshinori Akaishi, Toshimitsu Yamazaki·Oct 7, 2016SaveLearn
Feasibility study for the measurement of πN TDAs at PANDA in pp J/ψπ0The exclusive charmonium production process in pp annihilation with an associated π0 meson pp J/ψπ0 is studied in the framework of QCD collinear factorization. The feasibility…PANDA Collaboration, B. Singh, W. Erni et al.·Oct 7, 2016SaveLearn
First observation of a reactor-status effect on the beta+ decay rate of 22NaIn the search for an electron antineutrino detection method with sensitivity below the 1.8 MeV threshold for the inverse beta decay reaction, beta decay counting experiments with ca. 3 kBq 22Na and…Robert de Meijer, Albert Zondervan, Jan Stegenga et al.·Oct 5, 2016SaveLearn