41 research outputs found

    Antikaon Production in Proton-Nucleus Reactions and the K−K^- properties in nuclear matter

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    We calculate the momentum-dependent potentials for K+K^+ and K−K^- mesons in a dispersion approach at nuclear density ρ0\rho_0 using the information from the vacuum K+NK^+ N and K−NK^- N scattering amplitudes, however, leaving out the resonance contributions for the in-medium analysis. Whereas the K+K^+ potential is found to be repulsive (≈\approx + 30 MeV) and to show only a moderate momentum dependence, the K−K^- selfenergy at normal nuclear matter density turns out to be ≈\approx - 200 MeV at zero momentum in line with kaon atomic data, however, decreases rapidly in magnitude for higher momenta. The antikaon production in p + A reactions is calculated within a coupled transport approach and compared to the data at KEK including different assumptions for the antikaon potentials. Furthermore, detailed predictions are made for p+12Cp + ^{12}C and p+207Pbp + ^{207}Pb reactions at 2.5 GeV in order to determine the momentum dependent antikaon potential experimentally.Comment: 27 pages, LaTeX, including 14 ps-figures, UGI-98-1

    The Role of Lambda(1405) in Kaon-Proton Interactions

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    S-wave K−pK^-p scattering into various channels near threshold are analyzed in heavy-baryon chiral perturbation theory with Λ(1405)\Lambda (1405) introduced as an independent field. This is the approach that predicted the critical density 2<=ρc/ρ0<=32<=\rho_c/\rho_0 <=3 for negatively charged kaon condensation. We show that chiral perturbation expansion treating the Λ(1405)\Lambda (1405) as elementary is consistent with {\it all} threshold data including a double-charge-exchange process suppressed at leading order of chiral expansion in the absence of the Λ(1405)\Lambda (1405). We also discuss S-wave K+pK^+ p scattering phase shifts at low energy.Comment: 12 pages, epsfig.sty, 1 figure (uuencoded

    Vector Meson Mixing and Charge Symmetry Violation

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    We discuss the consistency of the traditional vector meson dominance (VMD) model for photons coupling to matter, with the vanishing of vector meson-meson and meson-photon mixing self-energies at q^2=0. This vanishing of vector mixing has been demonstrated in the context of rho-omega mixing for a large class of effective theories. As a further constraint on such models, we here apply them to a study of photon-meson mixing and VMD. As an example we compare the predicted momentum dependence of one such model with a momentum-dependent version of VMD discussed by Sakurai in the 1960's. We find that it produces a result which is consistent with the traditional VMD phenomenology. We conclude that comparison with VMD phenomenology can provide a useful constraint on such models.Comment: 7 pages, uses epsfig.sty. Publication details added to title pag

    Kaon-Nucleon Scattering from Chiral Lagrangians

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    The s-wave K±NK^{\pm}N scattering amplitude is computed up to one-loop order corresponding to next-to-next-to-leading order (or N2^2LO in short) with a heavy-baryon effective chiral Lagrangian. Constraining the low-energy constants by on-shell scattering lengths, we obtain contributions of each chiral order up to N2^2LO and find that the chiral corrections are ``natural" in the sense of viable effective field theories. We have also calculated off-shell ss-wave K−NK^-N scattering amplitudes relevant to kaonic atoms and K−K^- condensation in ``nuclear star" matter including the effect of Λ(1405)\Lambda (1405). The K−pK^-p amplitude is found to be quite sensitive to the intermediate Λ(1405)\Lambda (1405) contribution, while the K−nK^-n amplitude varies smoothly with the C.M. energy. The crossing-even one-loop corrections are found to play an important role in determining the higher-order chiral corrections.Comment: 14 pages and 2 figures(LaTeX), SNUTP-93-81. (References are added in the reference [21]

    Combined Description of N‟N\bf{\overline{N}N} Scattering and Annihilation With A Hadronic Model

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    A model for the nucleon-antinucleon interaction is presented which is based on meson-baryon dynamics. The elastic part is the GG-parity transform of the Bonn NNNN potential. Annihilation into two mesons is described in terms of microscopic baryon-exchange processes including all possible combinations of π,η,ρ,ω,a0,f0,a1,f1,a2,f2,K,K∗\pi,\eta,\rho,\omega,a_0,f_0,a_1,f_1,a_2,f_2,K,K^*. The remaining annihilation part is taken into account by a phenomenological energy- and state independent optical potential of Gaussian form. The model enables a simultaneous description of nucleon-antinucleon scattering and annihilation phenomena with fair quality.Comment: revised version, REVTEX, 9 pages, 10 figures available from this URL ftp://ikp113.ikp.kfa-juelich.de/pub/kph140/nucl-th.9411014.u

    Electromagnetic isoscalar rho-pi-gamma exchange current and the anomalous action

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    Using modern data, we first refit constants needed to complete an anomalous pi-rho-omega-a_1 Lagrangian obtained within the approach of hidden local symmetries. Then we derive from this Lagrangian electromagnetic isoscalar rho-pi-gamma and rho-a_1-gamma currents needed in calculations of the deuteron electromagnetic form factors at large momentum transfers.Comment: 16 pages, 1 figure, Latex, feynman, submitted to Nucl. Phys.

    X(1835) as the Lowest Mass Pseudoscalar Glueball and Proton Spin Problem

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    We consider the parity doublet structure observed in high hadronic excitations within the instanton model for the QCD vacuum. In the conventional approach this doubling phenomenon is treated as a manifestation of the partial restoration of chiral or U(1)AU(1)_A symmetry. We demonstrate that the suppression of direct instanton contribution to the masses of excited hadrons leads to the partial U(1)AU(1)_A symmetry restoration in hadron spectrum. The origin of X(1835) resonance observed by BES Collaboration is studied upon the doublet structure. We argue also how X(1835) be interpreted as the lowest pseudoscalar glueball state, and derive its coupling constant to proton. It turns out that this coupling is large and negative. Demonstrated is how this large coupling affects the gluonic contribution to the proton spin.Comment: 12 pages, LaTex, 1 eps-figure, expanded discussion on mechanism of parity doubling in high hadronic excitations, version to appear in Phys.Lett.

    The theory and phenomenology of polarized deep inelastic scattering

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    Comprehensive review paper on the theory and phenomenology of polarized deep inelastic scattering, to appear in Physics ReportsComment: 113 pages, latex, 40 figures not included (hard copies available via mail upon request to [email protected]
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