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Estimates for Fundamental Solutions of Second-Order Parabolic Equations
Journal of the London Mathematical Society, 2000zbMATH Open Web Interface contents unavailable due to conflicting licenses.
Liskevich, V, Semenov, Yu
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Homogenization for Degenerate Quasilinear Parabolic Equations of Second Order
Acta Mathematicae Applicatae Sinica, English Series, 2005zbMATH Open Web Interface contents unavailable due to conflicting licenses.
Zhang, Xingyou, Huang, Yong
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Removable singularities of solutions of second-order parabolic equations
Mathematical Notes of the Academy of Sciences of the USSR, 1991Let \({\mathcal L}\) denote a scalar linear second order parabolic operator on a bounded cylindrical domain \(Q\). Central in the paper is the notion of a set removable in a functional space \(Y\). By definition, it is a compact set \(E\subset Q\) such that if \(u\in Y\) is a weak solution of \({\mathcal L}u=0\) in \(Q\backslash E\) then necessarily ...
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LINEAR EQUATIONS OF THE SECOND ORDER OF PARABOLIC TYPE
Russian Mathematical Surveys, 1962CONTENTSIntroduction § 1. The maximum principle. Uniqueness of the solutions of the basic boundary value problems § 2. A priori estimates § 3. Solution of boundary value problems by Rothe's method. The Cauchy problem § 4. The fundamental solution of a linear parabolic equation. The Green's function.
A M Il'in, A S Kalashnikov, O A Oleinik
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Generalized solutions of second order parabolic equations
1966zbMATH Open Web Interface contents unavailable due to conflicting licenses.
Ivanov, A. V. +3 more
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Ito’s Second Order Parabolic Equations
19900.1. Let us fix T 0, T∈R + with T 0 ≤ T, and d, d 1 ∈N. Suppose that a standard probability space \( = (\Omega ,{\cal F},{\{ {{\cal F}_{t}}\} _{{t \in [0,T]}}},) \) and a standard Wiener process ω(t) in \( {^{{{d_{1}}}}} \) on this probability space are given.
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Second-Order Linear Parabolic Equations
1983Parabolic equations arise in diffusion processes, and more generally in “irreversible” time-dependent processes. Mathematically, this is reflected in the fact that the equations are not invariant under the reversal of time ; i.e., under the transformation t → —t. This means that knowledge about the “past” is lost as time increases.
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On Properties of Solutions to Nonlinear Parabolic Equations of the Second Order
Journal of Dynamical and Control Systems, 1999The author studies sufficient conditions for finite time blow-up of positive solutions of the equation \(u_t=Lu+a_0(x,t)u^{\sigma_1}\) in \(\Omega\times(0,T)\) satisfying the nonlinear boundary condition \({\partial u\over\partial\nu}=b_0(x,t)u^{\sigma_2}\).
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Degenerate elliptic‐parabolic equations of second order
Communications on Pure and Applied Mathematics, 1967Kohn, J. J., Nirenberg, Louis
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Asymptotic behaviour of the fundamental solution of a second-order parabolic equation
Sbornik: Mathematics, 1995Summary: We study the asymptotic behaviour as \(t \to \infty\) of the fundamental solution \(G(x,s,t)\) of the Cauchy problem for the parabolic equation \(G_t - G_{xx} + a(x)G = 0\), \(x \in \mathbb{R}^1\), \(t > 0\). We suppose that the coefficient \(a(x)\) can be written as \(x \to \pm \infty\) in the form \(a(x) = a_2^\pm x^{-2} + \varphi (x ...
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