2,466 research outputs found

    Universal factorized formula for the cross-section of two-particle scattering

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    We analyze the process of two-particle scattering with unstable particle in an intermediate state. It was shown that the cross-section can be represented in the universal factorized form for an arbitrary set of particles. Phenomenological analysis of factorization effect is fulfilled.Comment: 8 pages, corrected typos. change conten

    Basic Morphometric Characteristics for Antarctica and Budget of theAntarctic Ice Cover

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    On the foundation of the latest cartographical materials, obtained in the period of IGY and following years I. A. SUYETOVA carried out the complex of cartometrical works and received the following values : 1. The area of Antarctica. 2. The average altitude of the ice and rock surface in relation to the ocean level. 3. The volume and thickness of the ice of the ice sheet of Antarctica. 4. Perimeter of Antarctica. The valuation of the Antarctic perimeter as well as the latest glaciological facts allowed to make new attempts in calculating the budget of the Antarctic ice sheet. The analysis of facts necessary for calculation of the budget allowed to calculate maximum and average square miscalculations. The average square miscalculation shows the positive ice-budget of Antarctica. The valuation of the maximum miscalculation shows the equilibrium of ice in Antarctica

    Factorization effects in a model of unstable particles

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    The effects of factorization are considered within the framework of the model of unstable particles with a smeared mass. It is shown that two-particle cross section and three-particle decay width can be described by the universal factorized formulae for an unstable particles of an arbitrary spin in an intermediate state. The exact factorization is caused by the specific structure of the model unstable-particle propagators. This result is generalized to complicated scattering and decay-chain processes with unstable particles in intermediate states. We analyze applicability of the method and evaluate its accuracy.Comment: 13 pages, 7 figure

    Near-threshold boson pair production in the model of smeared-mass unstable particles

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    Near-threshold production of boson pairs is considered within the framework of the model of unstable particles with smeared mass. We describe the principal aspects of the model and consider the strategy of calculations including the radiative corrections. The results of calculations are in good agreement with LEP II data and Monte-Carlo simulations. Suggested approach significantly simplifies calculations with respect to the standard perturbative one.Comment: 15 pages, 6 figures, minor corrections, references adde

    Capture rate and neutron helicity asymmetry for ordinary muon capture on hydrogen

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    Applying heavy-baryon chiral perturbation theory to ordinary muon capture (OMC) on a proton, we calculate the capture rate and neutron helicity asymmetry up to next-to-next-to-leading order. For the singlet hyperfine state, we obtain the capture rate Gamma_0 = 695 sec^{-1} while, for the triplet hyperfine state, we obtain the capture rate Gamma_1 = 11.9 sec^{-1} and the neutron asymmetry alpha_1 = 0.93. If the existing formalism is used to relate these atomic capture rates to Gamma_{liq}, the OMC rate in liquid hydrogen, then Gamma_{liq} corresponding to our improved values of Gamma_0 and Gamma_1 is found to be significantly larger than the experimental value, primarily due to the updated larger value of g_A. We argue that this apparent difficulity may be correlated to the specious anomaly recently reported for mu^- + p to n + nu_mu + gamma, and we suggest a possibility to remove these two "problems" simply and simultaneously by reexamining the molecular physics input that underlies the conventional analysis of Gamma_{liq}.Comment: 14 pages, 1 figur

    QED Radiative Corrections in Processes of Exclusive Pion Electroproduction

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    Formalism for radiative correction (RC) calculation in exclusive pion electroproduction on the proton is presented. A FORTRAN code EXCLURAD is developed for the RC procedure. The numerical analysis is done in the kinematics of current Jefferson Lab experiments.Comment: 13 pages, 9 figures; requires RevTeX

    Low-Energy Compton Scattering of Polarized Photons on Polarized Nucleons

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    The general structure of the cross section of γN\gamma N scattering with polarized photon and/or nucleon in initial and/or final state is systematically described and exposed through invariant amplitudes. A low-energy expansion of the cross section up to and including terms of order ω4\omega^4 is given which involves ten structure parameters of the nucleon (dipole, quadrupole, dispersion, and spin polarizabilities). Their physical meaning is discussed in detail. Using fixed-t dispersion relations, predictions for these parameters are obtained and compared with results of chiral perturbation theory. It is emphasized that Compton scattering experiments at large angles can fix the most uncertain of these structure parameters. Predictions for the cross section and double-polarization asymmetries are given and the convergence of the expansion is investigated. The feasibility of the experimental determination of some of the struture parameters is discussed.Comment: 41 pages of text, 9 figures; minor revisions prior to publication in Phys. Rev.

    Towards the solution of the CP/CAC_{P}/C_{A} anomaly in shell-model calculations of muon capture

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    Recently many authors have performed shell-model calculations of nuclear matrix elements determining the rates of the ordinary muon capture in light nuclei. These calculations have employed well-tested effective interactions in large scale shell-model studies. For one of the nuclei of interest, namely 28^{28}Si, there exists recent experimental data which can be used to deduce the value of the ratio CP/CAC_{P}/C_{A} by using the calculated matrix elements. Surprisingly enough, all the abovementioned shell-model results suggest a very small value (0\simeq 0) for CP/CAC_{P}/C_{A}, quite far from the PCAC prediction and recent data on muon capture in hydrogen. We show that this rather disturbing anomaly is solved by employing effective transition operators. This finding is also very important in studies of the scalar coupling of the weak charged current of leptons and hadrons.Comment: Revtex, 6 pages, 2 figs include

    Radiative Corrections to γγttˉ\gamma\gamma\to t \bar t in the Electroweak Standard Model

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    The cross-section for γγttˉ\gamma\gamma\to t \bar t with arbitrary polarized photons is calculated within the electroweak Standard Model including the complete virtual and soft-photonic O(α)O(\alpha) corrections. We present a detailed numerical discussion of the radiative corrections with particular emphasis on the purely weak corrections. These are usually of the order of 1--10\% for energies up to 1 TeV. For unpolarized or equally polarized photons they reach almost 10\% close to threshold. The large corrections cannot be traced back to a universal origin like the running of α\alpha or the ρ\rho-parameter. Apart from the energy region around the Higgs resonance (γγHttˉ)(\gamma\gamma\to H^*\to t\bar t) the weak corrections are widely independent of the Higgs-boson mass.Comment: 22 pages, LaTeX (compressed, uuencoded), 20 figures as compressed uuencoded ps-files, complete ps-file available via anonymous ftp from ftp://ftp.physik.uni-wuerzburg.de/pub/preprint/WUE-ITP-95-017.p

    Magnetic-field-dependent zero-bias diffusive anomaly in Pb oxide-n-InAs structures: Coexistence of two- and three-dimensional states

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    The results of experimental and theoretical studies of zero-bias anomaly (ZBA) in the Pb-oxide-n-InAs tunnel structures in magnetic field up to 6T are presented. A specific feature of the structures is a coexistence of the 2D and 3D states at the Fermi energy near the semiconductor surface. The dependence of the measured ZBA amplitude on the strength and orientation of the applied magnetic field is in agreement with the proposed theoretical model. According to this model, electrons tunnel into 2D states, and move diffusively in the 2D layer, whereas the main contribution to the screening comes from 3D electrons.Comment: 8 double-column pages, REVTeX, 9 eps figures embedded with epsf, published versio
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