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Structure of nonnegative solutions for parabolic equations and perturbation theory for elliptic operators (Potential Theory and its related Fields)

机译：椭圆算子的抛物型方程非负解的结构和微扰理论（势理论及其相关领域）。

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MURATA Minoru;
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年度 2009
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正文语种 en
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机译：关于抛物线和椭圆形积分微分方程的L〜P理论
2. Maximum and anti-maximum principles and eigenfunctions estimates via perturbation theory of positive solutions of elliptic equations [J] . Yehuda Pinchover Mathematische Annalen . 1999,第3期

机译：通过椭圆方程正解的摄动理论估计最大和反最大原理和本征函数
3. Viscosity solutions of a degenerate parabolic-elliptic system arising in the mean-field theory of superconductivity [J] . Elliott CM., Stoth BEE., Schatzle E. Archive for Rational Mechanics and Analysis . 1998,第2期

机译：超导平均场理论中退化简并抛物线型椭圆系统的粘滞解
4. Analytic solution of the Schrodinger equation for H-like ions in strong laser fields treating the Coulomb potential exactly: the change of the ionization exponent beyond Keldysh's type theories [C] . Sergei Gordienko, Juergen Meyer-ter-Vehn European conference on laser interaction with matter . 2003

机译：Schrodinger方程对强激光场的H样离子的分析解决方案治疗库仑电位的精确激光电位：超越keldysh型理论之外的电离指数的变化
5. Topics in nonlinear elliptic equations: (1) Bifurcation theory of nonlinear elliptic equations; (2) Spike layer solutions of the Cahn-Hilliard equation. [D] . Shi, Junping. 1998

机译：非线性椭圆方程的主题：（1）非线性椭圆方程的分岔理论；（2）Cahn-Hilliard方程的尖峰层解。
6. EIGENFUNCTION EXPANSIONS FOR SINGULAR ELLIPTIC OPERATORS. II. THE HILBERT SPACE ARGUMENT; PARABOLIC EQUATIONS ON OPEN MANIFOLDS [O] . Felix E. Browder 1954

机译：奇异椭圆算子的本征函数展开式。二。希尔伯特空间论证；开流形上的抛物线方程
7. PARABOLIC EQUATIONS WHOSE NONNEGATIVE IN A CYLINDER ARE DETERMINED ONLY BY THEIR INITIAL VALUES(Potential Theory and its Related Fields) [O] . 石毛和弘, 村田實 1997

机译：圆柱中非负的抛物线方程仅由其初始值确定（势理论及其相关领域）
8. Theory of Nonlinear Diffusion of Plasma Across a Magnetic Field. I. Solution of a Class of Quasilinear Parabolic Equations. [R] . berryman,james g. 1976

机译：等离子体在磁场中的非线性扩散理论。一类拟线性抛物型方程的解。

Structure of nonnegative solutions for parabolic equations and perturbation theory for elliptic operators (Potential Theory and its related Fields)

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