12,301,376 research outputs found

    On unification of gravitation and electromagnetism in the framework of a general-relativistic approach

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    We consider the unification problem for the gravitational and electromagnetic interactions and its possible solution on the basis of the existence of an effective Riemannian space in nonlinear electrodynamicsComment: 3 pages, Talk given at the International Conference RUSGRAV-13, June 23-28, 2008, PFUR, Mosco

    A local gauge invariant infrared regularization of the Yang-Mills theory

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    A local gauge invariant infrared regularization for the Yang-Mills theory is constructed on the basis of a higher derivative formulation of the model.Comment: 7 page

    Multiphonon anharmonic decay of a quantum mode

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    A nonperturbative theory of multiphonon anharmonic transitions between energy levels of a local mode is presented. It is shown that the rate of transitions rearranges near the critical level number ncrn_{cr}: at smaller nn the process slows down, while at larger nn it accelerates in time, causing a jump-like loss of energy followed by the generation of phonon bursts. Depending on parameters, phonons are emitted in pairs, triplets etc.Comment: submitted to Europhys.Let

    Influence of high magnetic fields on superconducting transition of one-dimensional Nb and MoGe nanowires

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    The effects of strong magnetic field on superconducting Nb and MoGe nanowires with diameter 10\sim10 nm have been studied. We have found that the Langer-Ambegaokar-McCumber-Halperin (LAMH) theory of thermally activated phase slips is applicable in a wide range of magnetic fields and describes well the temperature dependence of the wire resistance, over eleven orders of magnitude. The field dependence of the critical temperature, TcT_{c}, extracted from the LAMH fits is in good quantitative agreement with the theory of pair-breaking perturbations that takes into account both spin and orbital contributions. The extracted spin-orbit scattering time agrees with an estimate τsoτ(c/Ze2)4\tau_{so}\simeq \tau(\hbar c/ Ze^{2})^{4}, where τ\tau is the elastic scattering time and ZZ is the atomic number.Comment: accepted for publication in Physical Review Letter
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