1,055 research outputs found

    Search for the eta-mesic helium at COSY

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    We review status and perspectives of the search of the eta-mesic helium at the cooler synchrotron COSY.Comment: Invited talk at the Excited QCD 09 Workshop, 8-14 February 2009, Zakopane, Poland, 6 page

    Combined analysis of the K+K−K^{+}K^{-} interaction using near threshold pp→ppK+K−pp \to ppK^+K^- data

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    The K+K−K^{+}K^{-} final state interaction was investigated based on both the K+K−K^{+}K^{-} invariant mass distributions measured at excess energies of Q = 10 and 28 MeV and the near threshold excitation function for the pp→ppK+K−pp \to ppK^{+}K^{-} reaction. The K+K−K^+K^- final state enhancement factor was parametrized using the effective range expansion. The effective range of the K+K−K^+K^- interaction was estimated to be: Re(bK+K−)=−0.1±0.4stat±0.3sysfm\mathrm{Re}(b_{K^{+}K^{-}}) = -0.1 \pm 0.4_{stat} \pm 0.3_{sys} \mathrm{fm} and Im(bK+K−)=1.2−0.2stat−0.0sys+0.1stat+0.2sysfm\mathrm{Im}(b_{K^{+}K^{-}}) = 1.2^{+0.1_{stat}+0.2_{sys}}_{-0.2_{stat}-0.0_{sys}} \mathrm{fm}, and the determined real and imaginary parts of the K+K−K^+K^- scattering length amount to: ∣Re(aK+K−)∣=8.0−4.0stat+6.0statfm|\mathrm{Re}(a_{K^{+}K^{-}})| = 8.0^{+6.0_{stat}}_{-4.0_{stat}} \mathrm{fm} and Im(aK+K−)=0.0−5.0stat+20.0statfm\mathrm{Im}(a_{K^{+}K^{-}}) = 0.0^{+20.0_{stat}}_{-5.0_{stat}} \mathrm{fm}.Comment: 5 pages, 3 figures, article accepted for publication in Phys. Rev.

    Search for the eta-mesic nuclei by means of COSY-11, WASA-at-COSY and COSY-TOF detector systems

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    We review status and perspectives of the search for the light eta-mesic nuclei using COSY-11, WASA-at-COSY and COSY-TOF detector systems.Comment: Invited talk at the International Symposium on Mesic Nuclei, Krakow, 16 June 201

    Test of charge conjugation invariance in the decay of the eta meson into pi(+)pi(-)pi(0)

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    In this work we present the preliminary results of the analysis of the pp->pp eta(->pp pi(+)pi(-)pi(0) reaction aiming to test the charge conjugation symmetry C in strong interactions. Based on approximately 10510^5 identified eta->pi(+)pi(-)pi(0) decay events we have extracted asymmetry parameters sensitive to C symmetry violation for different isospin values of the final state and we have established that all are consistent with zero within the obtained accuracy.Comment: MESON2012 - 12th International Workshop on Meson Production, Properties and Interactio

    Experimental proton-proton correlation function derived for the pp -> ppeta reaction

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    Based on the high statistics data from the pp -> ppX reaction measured by the COSY-11 collaboration [1] we have derived a two-proton correlation function for the production of the ppeta and pp+pions systems. The measured correlation function normalized to the value simulated for a point-like source was compared with a theoretical prediction in order to estimate the size of the reaction volume.Comment: Talk given at the Symposium on Meson Physics at COSY-11 and WASA-at-COSY Krakow, Poland, 17-22 June 200

    Luminosity determination for the quasi-free nuclear reactions

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    A method for the calculation of the luminosity for the proton-nucleus collisions based on the quasi-free proton-proton scattering is presented. As an example of application the integrated luminosity for the scattering of protons off the deuteron target is determined for the experiment of the quasi-free pn --> pneta reaction performed by means of the COSY-11 facility.Comment: 7 pages, 5 figures, Presented at Symposium on Meson Physics at COSY-11 and WASA-at-COSY, Cracow, Poland, 17-22 Jun 200

    Genuine Multipartite Entanglement in the 33-Photon Decay of Positronium

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    The electron-positron annihilation into two photons is a standard technology in medicine to observe e.g. metabolic processes in human bodies. A new tomograph will provide the possibility to observe not only direct e+e−e^+ e^- annihilations but also the 33 photons from the decay of ortho-positronium atoms formed in the body. We show in this contribution that the three-photon state with respect to polarisation degrees of freedom depends on the angles between the photons and exhibits various specific entanglement features. In particular genuine multipartite entanglement, a type of entanglement involving all degrees of freedoms, is subsistent if the positronium was in a definite spin eigenstate. Remarkably, when all spin eigenstates are mixed equally, entanglement --and even stronger genuine multipartite entanglement-- survives. Due to a "\textit{symmetrization}" process, however, DickeDicke-type of entanglement remains whereas GHZGHZ-type of entanglement vanishes. The survival of particular entanglement properties in the mixing scenario may make it possible to extract quantum information in form of distinct entanglement features, e.g., from metabolic processes in human bodies.Comment: 9 pages, 5 figure

    Multimeson production in pp interactions as a background for eta and eta' decays

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    Multimeson production in pp interactions comprises important background for eta, omega and eta' mesons production experiments and for the studies of their decays planned with WASA detector at COSY. The available information about the reactions is summarized and the need for efforts to describe the processes is stressed.Comment: Proceedings of MENU07 Conference Julich, Germany 200

    Luminosity determination for the deutron-deutron reactions using free and quasi-free reactions with WASA-at-COSY detector

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    Two methods of the luminosity determination for the experiment performed by WASA collaboration to search for 4−0.03cmHe^{4} {-0.03cm}{He}-η\eta bound state are presented. During the measurement the technique of continous change of the beam momentum in one accelerator cycle (called ramped beam) was applied. This imposes the requirement to determine not only the total integrated luminosity, but also its variation as a function of the beam momentum.Comment: Symposium on Applied Nuclear Physics and Innovative Technologies, Krakow (Poland), 24-27.09.201
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