84 research outputs found

    Sharp anisotropic estimates for the Boltzmann collision operator and its entropy production

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    This article provides sharp constructive upper and lower bound estimates for the non-linear Boltzmann collision operator with the full range of physical non cut-off collision kernels (γ>−n\gamma > -n and s∈(0,1)s\in (0,1)) in the trilinear L2(Rn)L^2(\R^n) energy . These new estimates prove that, for a very general class of g(v)g(v), the global diffusive behavior (on ff) in the energy space is that of the geometric fractional derivative semi-norm identified in the linearized context in our earlier works [2009, 2010, 2010 arXiv:1011.5441v1]. We further prove new global entropy production estimates with the same anisotropic semi-norm. This resolves the longstanding, widespread heuristic conjecture about the sharp diffusive nature of the non cut-off Boltzmann collision operator in the energy space L2(Rn)L^2(\R^n).Comment: 29 pages, updated file based on referee report; Advances in Mathematics (2011

    Recovery of time-dependent damping coefficients and potentials appearing in wave equations from partial data

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    We consider the inverse problem of determining a time-dependent damping coefficient aa and a time-dependent potential qq, appearing in the wave equation ∂t2u−Δxu+a(t,x)∂tu+q(t,x)u=0\partial_t^2u-\Delta_x u+a(t,x)\partial_tu+q(t,x)u=0 in Q=(0,T)×ΩQ=(0,T)\times\Omega, with T>0T>0 and Ω\Omega a C2 \mathcal C^2 bounded domain of Rn\mathbb R^n, n≥2n\geq2, from partial observations of the solutions on ∂Q\partial Q. More precisely, we look for observations on ∂Q\partial Q that allow to determine uniquely a large class of time-dependent damping coefficients aa and time-dependent potentials qq without involving an important set of data. We prove global unique determination of a∈W1,p(Q)a\in W^{1,p}(Q), with p>n+1p>n+1, and q∈L∞(Q)q\in L^\infty(Q) from partial observations on ∂Q\partial Q

    Determination of singular time-dependent coefficients for wave equations from full and partial data

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    We study the problem of determining uniquely a time-dependent singular potential qq, appearing in the wave equation ∂t2u−Δxu+q(t,x)u=0\partial_t^2u-\Delta_x u+q(t,x)u=0 in Q=(0,T)×ΩQ=(0,T)\times\Omega with T>0T>0 and Ω\Omega a C2 \mathcal C^2 bounded domain of Rn\mathbb R^n, n≥2n\geq2. We start by considering the unique determination of some singular time-dependent coefficients from observations on ∂Q\partial Q. Then, by weakening the singularities of the set of admissible coefficients, we manage to reduce the set of data that still guaranties unique recovery of such a coefficient. To our best knowledge, this paper is the first claiming unique determination of unbounded time-dependent coefficients, which is motivated by the problem of determining general nonlinear terms appearing in nonlinear wave equations
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