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Related papers: Hypernuclei Production by K- at rest

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Multiple polarization observables must be measured to access the amplitude structure of pseudoscalar meson photoproduction off the proton. The hyperon-producing reactions are especially attractive to study, since the weak decays allow…

Nuclear Experiment · Physics 2008-11-26 Reinhard Schumacher

In high-energy nuclear collisions, the new phase of the quark-gluon plasma is indicated by an anomalous increase in pressure, an excess of direct photon production, an excess of strangeness production, and an anomalous J/psi suppression. We…

Nuclear Theory · Physics 2011-08-11 Cheuk-Yin Wong

This PhD thesis is about the production of strange particles in heavy-ion collisions at high energy produced at the SPS CERN syncrotron. Results are from experiment WA85 and WA97. They have been compared with VENUS and RQMD simulations. An…

Nuclear Experiment · Physics 2007-05-23 Rocco Caliandro

The charged current one pion production induced by $\nu_\mu$ from nucleons and nuclei like $^{12}$C and $^{16}$O nuclei has been studied. The calculations have been done for the incoherent and the coherent processes from nuclear targets…

Nuclear Theory · Physics 2008-11-26 Shakeb Ahmad , M. Sajjad Athar , S. K. Singh

Strangeness (K$^{0,+}$, $\Lambda$ and $\Sigma^{-,0,+}$) production in heavy-ion collisions near threshold energies has been investigated within the Lanzhou quantum molecular dynamics (LQMD) transport model. The kaon (anti-kaon)-nucleon and…

Nuclear Theory · Physics 2015-06-17 Zhao-Qing Feng

In the framework of the nuclear spectral function approach for incoherent primary proton-nucleon and secondary pion-nucleon production processes we study the inclusive Lambda(1520) hyperon production in the interaction of 2.83 GeV protons…

Nuclear Theory · Physics 2011-11-10 E. Ya. Paryev

Since the pioneering experiment, E89-009 studying hypernuclear spectroscopy using the $(e,e^{\prime}K^+)$ reaction was completed, two additional experiments, E01-011 and E05-115, were performed at Jefferson Lab. These later experiments used…

Nuclear Experiment · Physics 2014-10-01 L. Tang , C. Chen , T. Gogami , D. Kawama , Y. Han , L. Yuan , A. Matsumura , Y. Okayasu , T. Seva , V. M. Rodriguez , P. Baturin , A. Acha , P. Achenbach , A. Ahmidouch , I. Albayrak , D. Androic , A. Asaturyan , R. Asaturyan , O. Ates , R. Badui , O. K. Baker , F. Benmokhtar , W. Boeglin , J. Bono , P. Bosted , E. Brash , P. Carter , R. Carlini , A. Chiba , M. E. Christy , L. Cole , M. M. Dalton , S. Danagoulian , A. Daniel , R. De Leo , V. Dharmawardane , D. Doi , K. Egiyan , M. Elaasar , R. Ent , H. Fenker , Y. Fujii , M. Furic , M. Gabrielyan , L. Gan , F. Garibaldi , D. Gaskell , A. Gasparian , E. F. Gibson , P. Gueye , O. Hashimoto , D. Honda , T. Horn , B. Hu , Ed V. Hungerford , C. Jayalath , M. Jones , K. Johnston , N. Kalantarians , H. Kanda , M. Kaneta , F. Kato , S. Kato , M. Kawai , C. Keppel , H. Khanal , M. Kohl , L. Kramer , K. J. Lan , Y. Li , A. Liyanage , W. Luo , D. Mack , K. Maeda , S. Malace , A. Margaryan , G. Marikyan , P. Markowitz , T. Maruta , N. Maruyama , V. Maxwell , D. J. Millener , T. Miyoshi , A. Mkrtchyan , H. Mkrtchyan , T. Motoba , S. Nagao , S. N. Nakamura , A. Narayan , C. Neville , G. Niculescu , M. I. Niculescu , A. Nunez , Nuruzzaman , H. Nomura , K. Nonaka , A. Ohtani , M. Oyamada , N. Perez , T. Petkovic , J. Pochodzalla , X. Qiu , S. Randeniya , B. Raue , J. Reinhold , R. Rivera , J. Roche , C. Samanta , Y. Sato , B. Sawatzky , E. K. Segbefia , D. Schott , A. Shichijo , N. Simicevic , G. Smith , Y. Song , M. Sumihama , V. Tadevosyan , T. Takahashi , N. Taniya , K. Tsukada , V. Tvaskis , M. Veilleux , W. Vulcan , S. Wells , F. R. Wesselmann , S. A. Wood , T. Yamamoto , C. Yan , Z. Ye , K. Yokota , S. Zhamkochyan , L. Zhu

We discuss strangeness production in heavy-ion collisions within and around the energy range of the planned NICA facility. We describe the minimal statistical model, in which the total strangeness yield is fixed by the observed or…

Nuclear Theory · Physics 2016-09-21 Boris Tomasik , E. E. Kolomeitsev

Production of single neutrinos as well as neutrino-antineutrino pairs by photons interacting with pseudo Nambu-Goldstone bosons is studied within the Standard Model. The corresponding cross sections are found analytically. The energy loss…

High Energy Physics - Phenomenology · Physics 2013-10-22 I. Alikhanov

Pronounced effects due to final state hyperon-nucleon interaction are predicted in strangeness photoproduction reaction on the deuteron. Use is made of the covariant reaction formalism and the P- matrix approach to the hyperon-nucleon…

High Energy Physics - Phenomenology · Physics 2009-10-31 B. Kerbikov

The strangeness-exchange reaction pi + Y -> K- + N is shown to be the dynamical origin of chemical equilibration for K- production in heavy-ion collisions up to beam energies of 10 A GeV. The hyperons occurring in this process are produced…

High Energy Physics - Phenomenology · Physics 2009-11-10 J. Cleymans , A. Foerster , H. Oeschler , K. Redlich , F. Uhlig

We have measured both yields of neutron-proton and neutron-neutron pairs emitted from the non-mesonic weak decay process of 5_Lambda-He and 12_Lambda-C hypernuclei produced via the (pi^+,K^+) reaction for the first time. We observed clean…

We investigate theoretically production cross sections of the $J^\pi=$ 0$^+$ ground state of a $^4_\Lambda$He hypernucleus in the $^4$He($\pi$,~$K$) reaction with a distorted-wave impulse approximation using the optimal Fermi-averaged $\pi…

Nuclear Theory · Physics 2019-09-04 Toru Harada , Yoshiharu Hirabayashi

Statistical hadronization is presented as mechanism for (strange) particle production from a deconfined quark--gluon plasma (QGP) fireball. We first consider hadronic resonance production at RHIC as a test of the model. We present in detail…

High Energy Physics - Phenomenology · Physics 2008-11-26 Jan Rafelski , Jean Letessier

Lambda*=Lambda(1405) plays an essential role in forming kaonic nuclear clusters (KNC). The simplest KNC, K-pp, has the structure Lambda*p=(K-p){I=0}p, where a real kaon migrates between two nucleons, mediating super-strong Lambda*-p$…

Nuclear Theory · Physics 2019-04-09 Y. Akaishi , T. Yamazaki

The collisions of large nuclei at high energies could produce metastable vacua which are odd under parity, P, charge conjugation, C, and/or CP. Using only the three-momenta of charged pions (or kaons), we show how to construct global…

High Energy Physics - Phenomenology · Physics 2009-10-31 Dmitri Kharzeev , Robert D. Pisarski

K$^{+}$K$^{-}$ pairs may be produced in photonuclear collisions, either from the decays of photoproduced $\phi (1020)$ mesons, or directly as non-resonant K$^{+}$K$^{-}$ pairs. Measurements of K$^{+}$K$^{-}$ photoproduction probe the…

Nuclear Experiment · Physics 2024-06-10 ALICE Collaboration

Low values of the fusion cross sections and very short half-lives of nuclei with Z$>$120 put obstacles in synthesis of new elements. Different nuclear reactions (fusion of stable and radioactive nuclei, multi-nucleon transfers and neutron…

Nuclear Theory · Physics 2015-06-05 Valeriy Zagrebaev , Alexander Karpov , Walter Greiner

We study the Glashow resonance $\bar{\nu}_e + e^- \rightarrow W^- \rightarrow$ hadrons at 6.3 PeV as diagnostic of the production processes of ultra-high energy neutrinos. The focus lies on describing the physics of neutrino production from…

High Energy Astrophysical Phenomena · Physics 2017-02-22 Daniel Biehl , Anatoli Fedynitch , Andrea Palladino , Tom J. Weiler , Walter Winter

The experimental results on the pion, strangeness and J/psi production in high energy nuclear collisions are discussed. The anomalous energy dependence of pion and strangeness production is consistent with the hypothesis that a transition…

High Energy Physics - Phenomenology · Physics 2015-06-25 Marek Gazdzicki
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