1,880 research outputs found

    Evolution of thick domain walls in inflationary and p=wρp=w\rho universe

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    We study the evolution of thick domain walls in the different models of cosmological inflation, in the matter-dominated and radiation-dominated universe, or more generally in the universe with the equation of state p=wρp=w\rho. We have found that the domain wall evolution crucially depends on the time-dependent parameter C(t)=1/(H(t)ÎŽ0)2C(t)=1/(H(t)\delta_0)^2, where H(t)H(t) is the Hubble parameter and ÎŽ0\delta_0 is the thickness of the wall in flat space-time. For C(t)>2C(t)>2 the physical thickness of the wall, a(t)ÎŽ(t)a(t)\delta(t), tends with time to ÎŽ0\delta_0, which is microscopically small. Otherwise, when C(t)≀2C(t) \leq 2, the wall steadily expands and can grow up to a cosmologically large size.Comment: 15 pages, 9 figure

    Reminiscences about numerical schemes

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    This preprint appeared firstly in Russian in 1997. Some truncated versions of this preprint were published in English and French, here a fully translated version is presented. The translation in English was done by O. V. Feodoritova and V. Deledicque to whom I express my gratitude

    Suppression of H→VVH\to VV decay channels in the Georgi-Machacek model

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    The H→ZZH\to ZZ decay mode is usually considered as one of the most promising ways to discover new heavy neutral scalar HH. We show that in the Georgi-Machacek model it is possible to get large enhancement of double SM-like Higgs boson production due to HH decays while ZZZZ and WWWW decay channels could be highly suppressed.Comment: 5 page

    A unified hyperbolic formulation for viscous fluids and elastoplastic solids

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    We discuss a unified flow theory which in a single system of hyperbolic partial differential equations (PDEs) can describe the two main branches of continuum mechanics, fluid dynamics, and solid dynamics. The fundamental difference from the classical continuum models, such as the Navier-Stokes for example, is that the finite length scale of the continuum particles is not ignored but kept in the model in order to semi-explicitly describe the essence of any flows, that is the process of continuum particles rearrangements. To allow the continuum particle rearrangements, we admit the deformability of particle which is described by the distortion field. The ability of media to flow is characterized by the strain dissipation time which is a characteristic time necessary for a continuum particle to rearrange with one of its neighboring particles. It is shown that the continuum particle length scale is intimately connected with the dissipation time. The governing equations are represented by a system of first order hyperbolic PDEs with source terms modeling the dissipation due to particle rearrangements. Numerical examples justifying the reliability of the proposed approach are demonstrated.Comment: 6 figure

    Eigenvalue enclosures and exclosures for non-self-adjoint problems in hydrodynamics

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    In this paper we present computer-assisted proofs of a number of results in theoretical fluid dynamics and in quantum mechanics. An algorithm based on interval arithmetic yields provably correct eigenvalue enclosures and exclosures for non-self-adjoint boundary eigenvalue problems, the eigenvalues of which are highly sensitive to perturbations. We apply the algorithm to: the Orr-Sommerfeld equation with Poiseuille profile to prove the existence of an eigenvalue in the classically unstable region for Reynolds number R=5772.221818; the Orr-Sommerfeld equation with Couette profile to prove upper bounds for the imaginary parts of all eigenvalues for fixed R and wave number α; the problem of natural oscillations of an incompressible inviscid fluid in the neighbourhood of an elliptical flow to obtain information about the unstable part of the spectrum off the imaginary axis; Squire's problem from hydrodynamics; and resonances of one-dimensional Schrödinger operators

    Entropy Balance and Dispersive Oscillations in Lattice Boltzmann Models

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    We conduct an investigation into the dispersive post-shock oscillations in the entropic lattice-Boltzmann method (ELBM). To this end we use a root finding algorithm to implement the ELBM which displays fast cubic convergence and guaranties the proper sign of dissipation. The resulting simulation on the one-dimensional shock tube shows no benefit in terms of regularization from using the ELBM over the standard LBGK method. We also conduct an experiment investigating of the LBGK method using median filtering at a single point per time step. Here we observe that significant regularization can be achieved.Comment: 18 pages, 4 figures; 13/07/2009 Matlab code added to appendi

    Extending the Higgs sector: an extra singlet

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    An extension of the Standard Model with an additional Higgs singlet is analyzed. Bounds on singlet admixture in 125 GeV h boson from electroweak radiative corrections and data on h production and decays are obtained. Possibility of double h production enhancement at 14 TeV LHC due to heavy higgs contribution is considered.Comment: 18 pages, 7 figures. v2: one equation added; references received after the publication of v1 are adde
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