6,527,385 research outputs found

    Lightest scalar and tensor resonances in γγππ\gamma\gamma\to\pi\pi after the Belle experiment

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    New high statistics Belle data on the γγπ+π\gamma\gamma\to\pi^+\pi^- reaction cross section measured in the range of pion-pair invariant masses s\sqrt{s} between 0.8 GeV and 1.5 GeV are analyzed to clarify the current situation around the σ(600)\sigma(600), f0(980)f_0(980), and f2(1270)f_2(1270) resonances in γγ\gamma\gamma collisions. The present analysis shows that the direct coupling constants of the σ(600)\sigma(600) and f0(980)f_0(980) resonances to γγ\gamma\gamma are small, and the σ(600)γγ\sigma(600)\to\gamma\gamma and f0(980)γγf_0(980)\to\gamma\gamma decays are four-quark transitions caused by the π+π\pi^+\pi^- and K+KK^+K^- loop mechanisms, respectively. The chiral shielding of the σ(600)\sigma(600) resonance takes place in the reactions γγππ\gamma\gamma\to\pi\pi as well as in ππ\pi\pi scattering. Some results of a simultaneous description of the γγπ+π\gamma\gamma\to\pi^+\pi^- and γγπ0π0\gamma\gamma\to\pi^0\pi^0 Belle data are also presented. In particular, the following tentative estimate of the f2(1270)γγf_2(1270)\to\gamma\gamma decay width is obtained: Γf2γγ(mf22)3.68\Gamma_{f_2\to\gamma\gamma}(m^2_{f_2})\approx 3.68 keV.Comment: 14 pages, 5 figures. Fitted for the publication in Physical Review

    The analytical ππ\pi\pi scattering amplitude and the light scalars

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    In this work we construct the ππ\pi\pi scattering amplitude T00T^0_0 with regular analytical properties in the ss complex plane, which describes simultaneously the data on the ππ\pi\pi scattering, ϕπ0π0γ\phi\to\pi^0\pi^0\gamma decay, and ππKKˉ\pi\pi\to K\bar K reaction. The chiral shielding of the σ(600)\sigma (600) meson and its mixing with the f0(980)f_0(980) meson are also taken into account. The data agrees with the four-quark nature of the σ(600)\sigma (600) and f0(980)f_0(980) mesons. The amplitude in the range 5mπ2<s<0.64-5 m_\pi^2 < s < 0.64 GeV2^2 also agrees with results, obtained on the base of the chiral expansion, dispersion relations, and the Roy equations.Comment: Published version: a few clarifications are added, the Editors corrections are taken into accoun

    The Running BFKL: Resolution of Caldwell's Puzzle

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    The HERA data on the proton structure function, F2(x,Q2)F_2(x,Q^2), at very small xx and Q2Q^2 show the dramatic departure of the logarithmic slope, F2/logQ2\partial F_2/\partial\log Q^2, from theoretical predictions based on the DGLAP evolution. We show that the running BFKL approach provides the quantitative explanation for the observed xx and/or Q2Q^2 -dependence of F2/logQ2\partial F_2/\partial\log Q^2.Comment: 7 pages, Latex, 4 Figures, P

    Light Scalar Mesons as Manifestation of Spontaneously Broken Chiral Symmetry

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    Attention is paid to the production mechanisms of light scalars that reveal their nature. We reveal the chiral shielding of the \sigma(600) meson. We show that the kaon loop mechanism of the \phi radiative decays, ratified by experiment, points to the four-quark nature of light scalars. We show also that the light scalars are produced in the two photon collisions via four-quark transitions in contrast to the classic P wave tensor q\bar q mesons that are produced via two-quark transitions γγqqˉ\gamma\gamma\to q\bar q. The history of spontaneous breaking of symmetry in quantum physics is discussed in Appendix.Comment: Talk at The International Bogolyubov Conference "Problems of Theoretical and Mathematical Physics" devoted to the 100th anniversary of N.N.Bogolyubov's birth that was held from August 21 to August 22,2009 in Moscow at the Russian Academy of Sciences (RAS) and from August 23 to August 27, 2009 in Dubna at the Joint Institute for Nuclear Research (JINR

    Unifying aspects of polarization of vector mesons from hard production in DIS and at Tevatron

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    Virtual photons have both the transverse and longitudinal polarization. In the inclusive DIS the impact of longitudinal photons, quantified by R=sigmaL/\igmaT sim 0.2, is marginal, but in diffractive DIS with excitation of small mass hadronic states or exclusive diffraction into vector mesons, QCD predicts R >> 1 in agreement with the experiment. After a brief review of the modern status of QCD theory of diffractive vector meson production I argue that longitudinally polarized gluons give rise to a large longitudinal polarization of the prompt JPsi and Psiprim observed at the Tevatron.Comment: Conference on Perspectives in Hadronic Physics (7 - 11 May 2001), ICTP, Trieste, Ital

    Gapless Hartree-Fock-Bogoliubov Approximation for Bose Gases

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    A dilute Bose system with Bose-Einstein condensate is considered. It is shown that the Hartree-Fock-Bogolubov approximation can be made both conserving as well as gapless. This is achieved by taking into account all physical normalization conditions, that is, the normalization condition for the condensed particles and that for the total number of particles. Two Lagrange multipliers, introduced for preserving these normalization conditions, make the consideration completely self-consistent.Comment: Latex file, 22 pages, 2 figure

    Covariant Matrix Model of Superparticle in the Pure Spinor Formalism

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    On the basis of the Berkovits pure spinor formalism of covariant quantization of supermembrane, we attempt to construct a M(atrix) theory which is covariant under SO(1,10)SO(1,10) Lorentz group. We first construct a bosonic M(atrix) theory by starting with the first-order formalism of bosonic membrane, which precisely gives us a bosonic sector of M(atrix) theory by BFSS. Next we generalize this method to the construction of M(atrix) theory of supermembranes. However, it seems to be difficult to obtain a covariant and supersymmetric M(atrix) theory from the Berkovits pure spinor formalism of supermembrane because of the matrix character of the BRST symmetry. Instead, in this paper, we construct a supersymmetric and covariant matrix model of 11D superparticle, which corresponds to a particle limit of covariant M(atrix) theory. By an explicit calculation, we show that the one-loop effective potential is trivial, thereby implying that this matrix model is a free theory at least at the one-loop level.Comment: 13 pages, no figures, two references adde
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