18,124 research outputs found

    On the structure of large N cancellations in baryon chiral perturbation theory

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    We show how to compute loop graphs in heavy baryon chiral perturbation theory including the full functional dependence on the ratio of the Delta--nucleon mass difference to the pion mass, while at the same time automatically incorporating the 1/N cancellations that follow from the large-N spin-flavor symmetry of baryons in QCD. The one-loop renormalization of the baryon axial vector current is studied to demonstrate the procedure. A new cancellation is identified in the one-loop contribution to the baryon axial vector current. We show that loop corrections to the axial vector currents are exceptionally sensitive to deviations of the ratios of baryon-pion axial couplings from SU(6) values

    HIV testing and informed consent - ethical considerations

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    One of the authors (T.J.) was invited by the AIDS Advisory Group to form a widely representative committee to recommend ethical guidelines concerning the extent to which HIV testing should receive informed consent. This paper presents and argues for the recommended guidelines. The question is considered with regard to a number of distinct purposes of HIV testing: the care of a patient; research; blood, tissue and organ donation; and the protection of third parties, including the health care worker. We contend that in each case there is no good reason for the requirement of informed consent to be significantly waived

    Spin-Flavor Structure of Large N Baryons

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    The spin-flavor structure of large N baryons is described in the 1/N expansion of QCD using quark operators. The complete set of quark operator identities is obtained, and used to derive an operator reduction rule which simplifies the 1/N expansion. The operator reduction rule is applied to the axial currents, masses, magnetic moments and hyperon non-leptonic decay amplitudes in the SU(3)SU(3) limit, to first order in SU(3)SU(3) breaking, and without assuming SU(3)SU(3) symmetry. The connection between the Skyrme and quark representations is discussed. An explicit formula is given for the quark model operators in terms of the Skyrme model operators to all orders in 1/N1/\N for the two flavor case.Comment: 36 pages, 2 eps figures, uses revte

    Renormalization of the baryon axial vector current in large-N_c chiral perturbation theory

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    The baryon axial vector current is computed at one-loop order in heavy baryon chiral perturbation theory in the large-N_c limit, where N_c is the number of colors. Loop graphs with octet and decuplet intermediate states cancel to various orders in N_c as a consequence of the large-N_c spin-flavor symmetry of QCD baryons. These cancellations are explicitly shown for the general case of N_f flavors of light quarks. In particular, a new generic cancellation is identified in the renormalization of the baryon axial vector current at one-loop order. A comparison with conventional heavy baryon chiral perturbation theory is performed at the physical values N_c=3, N_f=3.Comment: REVTex4, 29 pages, 2 figures, 6 tables. Equations (32) and (81) corrected. Some typos fixed. Results and conclusions remain unchange

    Large N_c, Constituent Quarks, and N, Delta Charge Radii

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    We show how one may define baryon constituent quarks in a rigorous manner, given physical assumptions that hold in the large-N_c limit of QCD. This constituent picture gives rise to an operator expansion that has been used to study large-N_c baryon observables; here we apply it to the case of charge radii of the N and Delta states, using minimal dynamical assumptions. For example, one finds the relation r_p^2 - r_{Delta^+}^2 = r_n^2 - r_{Delta^0}^2 to be broken only by three-body, O(1/N_c^2) effects for any N_c.Comment: 15 pages, 1 eps figure. Version to appear in Phys. Rev.

    Chiral Perturbation Theory for τρπντ\tau \to \rho \pi\nu_\tau, τKπντ\tau \to K^* \pi \nu_\tau, and τωπντ\tau \to \omega \pi \nu_\tau

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    We use heavy vector meson SU(2)L×SU(2)RSU(2)_L \times SU(2)_R chiral perturbation theory to predict differential decay distributions for τρπντ\tau \rightarrow \rho \pi \nu_\tau and τKπντ\tau \rightarrow K^* \pi \nu_\tau in the kinematic region where pVpπ/mVp_V \cdot p_\pi/m_V (here V=ρV = \rho or KK^*) is much smaller than the chiral symmetry breaking scale. Using the large number of colors limit we also predict the rate for τωπντ\tau \rightarrow \omega \pi \nu_\tau in this region (now V=ωV = \omega). Comparing our prediction with experimental data, we determine one of the coupling constants in the heavy vector meson chiral Lagrangian.Comment: 14 pages, latex 2e. We include the decay of the tau into the omega, pi minus and the tau neutrino, and extract a value for the coupling constant g2, using experimental dat

    Electromagnetic Moments of the Baryon Decuplet

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    We compute the leading contributions to the magnetic dipole and electric quadrupole moments of the baryon decuplet in chiral perturbation theory. The measured value for the magnetic moment of the Ω\Omega^- is used to determine the local counterterm for the magnetic moments. We compare the chiral perturbation theory predictions for the magnetic moments of the decuplet with those of the baryon octet and find reasonable agreement with the predictions of the large--NcN_c limit of QCD. The leading contribution to the quadrupole moment of the Δ\Delta and other members of the decuplet comes from one--loop graphs. The pionic contribution is shown to be proportional to IzI_z (and so will not contribute to the quadrupole moment of I=0I=0 nuclei), while the contribution from kaons has both isovector and isoscalar components. The chiral logarithmic enhancement of both pion and kaon loops has a coefficient that vanishes in the SU(6)SU(6) limit. The third allowed moment, the magnetic octupole, is shown to be dominated by a local counterterm with corrections arising at two loops. We briefly mention the strange counterparts of these moments.Comment: Uses harvmac.tex, 15 pages with 3 PostScript figures packed using uufiles. UCSD/PTH 93-22, QUSTH-93-05, Duke-TH-93-5
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