65 research outputs found

    TAU-PAIR PRODUCTION VIA PHOTON-PHOTON COLLISIONS AT LEP

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    We point out that the cross-section for the process e+e−→e+e−τ+τ−e^+ e^- \to e^+ e^- \tau^+ \tau^- at LEP is large enough to allow for a study of the anomalous electromagnetic couplings of the τ\tau lepton. We show that the present bounds on the magnetic dipole moment can be improved and that competitive bounds can be obtained for the electric dipole moment using the data taken from 1992 to 1994. Finally, we briefly discuss the improvements that can be obtained at LEP II.Comment: 9 pages, latex, 2 figure

    Weak magnetic dipole moments in two-Higgs-doublet models

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    We investigate the effects of the new scalars in a two-Higgs-doublet model on the weak magnetic dipole moments of the fermions at the ZZ peak. Proportionality of the Yukawa couplings to the fermion masses, and to tan⁥ÎČ\tan{\beta}, makes such effects more important for the third family, and potentially relevant. For the τ\tau lepton, the new diagrams are suppressed by vτ=2sin⁥2ΞW−1/2v_\tau = 2 \sin^2 \theta_W - 1/2, or by powers of mτ/MZm_\tau/M_Z, but may still be comparable to the SM electroweak contributions. In contrast, we find that the new contributions for the bottom quark may be much larger than the SM electroweak contributions. These new effects may even compete with the gluonic contribution, if the extra scalars are light and tan⁥ÎČ\tan \beta is large. We also comment on the problem of the gauge dependence of the vertex, arising when the ZZ is off mass shell. We compute the contributions from the new scalars to the magnetic dipole moments for top-quark production at the NLC, and for bottom and τ \tau production at LEP2. In the case of the top, we find that the SM electroweak and gluonic contributions to the ZttˉZ t {\bar t} vertex are comparable. The new contributions may be of the same order of magnitude as the standard-model ones, but not much larger.Comment: 17 pages, LaTex, 8 figures available upon reques

    Can We Observe Weak Anomalous Couplings of Heavy Quarks Through Three Jet Events?

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    The rates and corresponding jet distributions for the decay Z→bbˉgZ\to b\bar bg and the process e+e−→ttˉge^+e^-\to t\bar tg may be sensitive to anomalous dipole-like couplings of heavy quarks to the photon and ZZ. In the bb-quark case, after updating our previous analysis on the constraints imposed by current experiments on ZbbˉZb\bar b anomalous couplings, we show that the variation of these couplings within their presently allowed ranges leads to rather minor modifications to the Standard Model expectations for Z→bbˉgZ\to b\bar bg observables. In the tt-quark case, significant deviations from the Standard Model predictions for ttˉgt\bar tg production at the Next Linear Collider are possible.Comment: 26 pages with 9 embedded figures; gzipped, uuencoded postscript file. To obtain a copy of this paper send e-mail to [email protected]

    A consistent treatment for pion form factors in space-like and time-like regions

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    We write down some relevant matrix elements for the scattering and decay processes of the pion by considering a quark-meson vertex function. The pion charge and transition form factors FπF_\pi, FÏ€ÎłF_{\pi\gamma}, and FÏ€Îłâˆ—F_{\pi\gamma^*} are extracted from these matrix elements using a relativistic quark model on the light-front. We found that, the form factors FπF_\pi and FÏ€ÎłF_{\pi\gamma} in the space-like region agree well with experiment. Furthermore, the branching ratios of all observed decay modes of the neutral pion, that are related to the form factors FÏ€ÎłF_{\pi\gamma} and FÏ€Îłâˆ—F_{\pi\gamma^*} in the time-like region, are all consistent with the data as well. Additionally, FπF_\pi in the time-like region, which deals with the nonvalence contribution, is also discussed.Comment: 24 pages, 6 figures, to appear in Phys. Rev.

    Mapeamento de coletas antigas de acessos de espécies forrageiras nativas do Sul do Brasil.

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    O trabalho consistiu na anĂĄlise de cadernetas de coleta de campo antigas da Embrapa PecuĂĄria Sul, compilando os dados de longitude, atitude e altitude de 205 acessos de Bromus auleticus, Paspalum dilatatum, P. notatum, P. pumilum e P. urvillei.Zootec

    W ANOMALOUS MOMENTS AND THE POLARIZATION ASYMMETRY ZERO IN gamma e --> W nu

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    We show from general principles that there must be a center of mass energy, s0\sqrt s_0, where the polarization asymmetry A=Δσ(Îłe→WÎœ)/σ(Îłe→WÎœ)A=\Delta \sigma({\gamma e \to W \nu })/ \sigma({\gamma e \to W \nu }) for circularly-polarized photon and electron beams vanishes. In the case of the Standard Model, the crossing point where the asymmetry changes sign occurs in Born approximation at sÎłe=3.1583
MW≃254\sqrt s_{\gamma e} = 3.1583\ldots M_W \simeq 254 GeV. We demonstrate the sensitivity of the position of the polarization asymmetry zero to modifications of the SM trilinear ÎłWW\gamma W W coupling. Given reasonable assumptions for the luminosity and energy range for the Next Linear Collider(NLC) with a backscattered laser beam, we show that the zero point, s0\sqrt s_0, of the polarization asymmetry may be determined with sufficient precision to constrain the anomalous couplings of the WW to better than the 1\% level at 95%95\% CL. In addition to the fact that only a limited range of energy is required, the polarization asymmetry measurements have the important advantage that many of the systematic errors cancel in taking cross section ratios. The position of the zero thus provides an additional weapon in the arsenal used to probe anomalous trilinear gauge couplings.Comment: 21 pages, uuencoded postscript file. For hard copy, send e-mail to [email protected]

    Search for Manifestations of New Physics in Fermion-Pair Production at LEP

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    The measurements of hadron and lepton-pair production cross sections and leptonic forward-backward asymmetries performed with the L3 detector at centre-of-mass energies between 130 GeV and 189 GeV are used to search for new physics phenomena such as: contact interactions, exchange of virtual leptoquarks, scalar quarks and scalar neutrinos, effects of TeV strings in models of quantum gravity with large extra dimensions and non-zero sizes of the fermions. No evidence for these phenomena is found and new limits on their parameters are set

    Polarized \Lambda_b \to X_c \tau \nu in the SM and THDM

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    The inclusive rate and τ\tau spectrum for a polarized Λb\Lambda_b -baryon to decay to charm hadronic final states and leptons Ï„Îœ\tau \nu in the SM and a two-Higgs doublet model are computed.The O(αs)O(\alpha_s) QCD corrections to τ\tau spectrum in the two-Higgs model are also given.Comment: Revtex,11 pages,5 figure

    eta-prime Meson Production in Nucleon-Nucleon Collisions Near The Threshold

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    The production of ηâ€Č\eta' mesons in the reactions pp→ppηâ€Čpp\to pp\eta' and pn→pnηâ€Čpn\to pn\eta' at threshold-near energies is analyzed within a covariant effective meson-nucleon theory. The description of cross section and angular distributions of the available data in this kinematical region in the pppp channel is accomplished by including meson currents and nucleon currents with the resonances S11(1650)S_{11}(1650), P11(1710)P_{11}(1710) and P13(1720)P_{13}(1720). Predictions for the pnpn channel are given. The di-electron production from subsequent ηâ€Č\eta' Dalitz decay ηâ€Č→γγ∗→γe+e−\eta' \to \gamma \gamma^* \to\gamma e^+e^- is also calculated and numerical results are presented for intermediate energy and kinematics of possible experiments with HADES, CLAS and KEK-PS
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