26,280 research outputs found

    Induced pseudoscalar form factor of the nucleon at two-loop order in chiral perturbation theory

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    We calculate the imaginary part of the induced pseudoscalar form factor of the nucleon GP(t)G_P(t) in the framework of two-loop heavy baryon chiral perturbation theory. The effect of the calculated three-pion continuum on the pseudoscalar constant gP=(mμ/2M)GP(t=0.877mμ2)g_P = (m_\mu/2M) G_P(t=-0.877m_\mu^2) measurable in ordinary muon capture μpνμn\mu^-p\to \nu_\mu n turns out to be negligibly small. Possible contributions from counterterms at two-loop order are numerically smaller than the uncertainty of the dominant pion-pole term proportional to the pion-nucleon coupling constant gπN=13.2±0.2g_{\pi N}= 13.2\pm 0.2. We conclude that a sufficiently accurate representation of the induced pseudoscalar form factor of the nucleon at low momentum transfers tt is given by the sum of the pion-pole term and the Adler-Dothan-Wolfenstein term: GP(t)=4gπNMfπ/(mπ2t)2gAM2/3G_P(t) = 4g_{\pi N} M f_\pi/ (m_\pi^2 -t)- 2g_A M^2 /3, with =(0.44±0.02) = (0.44 \pm 0.02) fm2^2 the axial mean square radius of the nucleon.Comment: 6 pages, 2 figures, accepted for publication in Physical Review

    On the analysis of the pion--nucleon σ\sigma--term: The size of the remainder at the Cheng--Dashen point

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    We calculate the one--loop contributions of order Mπ4M_\pi^4 to the difference ΔR\Delta_R between the on--shell pion--nucleon scattering amplitude Dˉ+(0,2Mπ2)\bar{D}^+(0,2M_\pi^2) at the Cheng--Dashen point ν=0\nu =0, t=2Mπ2t=2M_\pi^2 and the scalar form factor σ(2Mπ2)\sigma (2M_\pi^2) in the framework of heavy baryon chiral perturbation theory. We proof that to this order ΔR\Delta_R contains nono chiral logarithms and therefore it vanishes simply as Mπ4M_\pi^4 in the chiral limit. Numerically, we find as an upper limit ΔR2\Delta_R \simeq 2\,MeV.Comment: 7 pp, LaTeX, uses epsf, 1 figure in separate PS fil

    Poisson algebra of 2d dimensionally reduced gravity

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    Using a Lax pair based on twisted affine sl(2,R)sl(2,R) Kac-Moody and Virasoro algebras, we deduce a r-matrix formulation of two dimensional reduced vacuum Einstein's equations. Whereas the fundamental Poisson brackets are non-ultralocal, they lead to pure c-number modified Yang-Baxter equations. We also describe how to obtain classical observables by imposing reasonable boundaries conditions.Comment: 16 pages, minor corrections. To appear in JHE

    Double neutral pion photoproduction at threshold

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    We consider the chiral expansion of the threshold amplitude for the reaction γpπ0π0p\gamma p \to \pi^0 \pi^0 p to order O(Mπ2){\cal O}(M_\pi^2). We substantiate a claim that this photoproduction channel is significantly enhanced close to threshold due to pion loops. A precise measurement of the corresponding cross sections is called for which allows to test chiral perturbation theory.Comment: 8 pp, LaTe

    Partially Quenched QCD with Non-Degenerate Dynamical Quarks

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    We discuss the importance of using partially quenched theories with three degenerate quarks for extrapolating to QCD, and present some relevant results from chiral perturbation theory.Comment: LATTICE99 talk. 3 pages, 2 figures. Uses epsf and espcrc2.st

    Threshold Two-Pion Photo- and Electroproduction: More neutrals than expected

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    We present an exploratory study of two pion photo-- and electroproduction off the nucleon in the threshold region. To calculate the pertinent amplitudes, we make use of heavy baryon chiral perturbation theory. We show that due to finite chiral loops the production cross section for final states with two neutral pions is considerably enhanced. The experimental implications are briefly discussed.Comment: 23pp, plain TeX, 11 figures available upon request, CRN 94/1

    Low--Energy Theorems for Weak Pion Production

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    We derive novel low--energy theorems for single pion production off nucleons through the isovector axial current. We find that the k2k^2-dependence of the multipole L0+(+)L_{0+}^{(+)} at threshold is given by the nucleon scalar form factor, namely σ(k2Mπ2)/(3πMπFπ)\sigma(k^2-M_\pi^2 ) /(3 \pi M_\pi F_\pi ). The relation to PCAC results for soft pions including electroweak form factors is also clarified.Comment: 9 pp, TeX, 2 figures available as ps files, CRN 93-5

    The Reaction πNππN\pi N \to \pi \pi N at Threshold

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    We consider the chiral expansion for the reaction πNππN\pi N \to \pi \pi N in heavy baryon chiral perturbation theory. To order MπM_\pi we derive novel low--energy theorems that compare favorably with recent determinations of the total cross sections for π+pπ+π+n\pi^+ p \to \pi^+ \pi^+ n and πpπ0π0n\pi^- p \to \pi^0 \pi^0 n.Comment: 7 pp, LateX (uses epsf.sty), 3 figures appended as ps files (split off as ppnf1.ps,ppnf2.ps,ppnf3.ps), CRN 94/1

    New Developments in Gaming Taxation and Regulation: an Update

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    The gaming industry is facing increased regulatory interest. Congress has authorized a commission to investigate gaming in the United States. The Internal Revenue Service continues to interpret ambiguous areas of the tax code in an attempt to raise gaming tax revenues. Regulatory changes in currency transaction reporting have also resulted in some significant changes for the industry. The purpose of this paper is to provide an update on tax and regulatory issues currently facing the gaming industry. Specifically, the paper will address tax and regulatory developments in: (a) tip compliance, (b) cash transaction reporting, (c) complimentaries, (d) employee cafeterias, (e) outstanding chips and tokens, (e) marker discounts, and (f) high-denomination slot win reporting
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