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Titlebook: Analysis IV; Linear and Boundary V. G. Maz’ya,S. M. Nikol’ski? Book 1991 Springer-Verlag Berlin Heidelberg 1991 Integralgleichungen.Nichts

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期刊全稱Analysis IV
期刊簡稱Linear and Boundary
影響因子2023V. G. Maz’ya,S. M. Nikol’ski?
視頻videohttp://file.papertrans.cn/157/156140/156140.mp4
學(xué)科分類Encyclopaedia of Mathematical Sciences
圖書封面Titlebook: Analysis IV; Linear and Boundary  V. G. Maz’ya,S. M. Nikol’ski? Book 1991 Springer-Verlag Berlin Heidelberg 1991 Integralgleichungen.Nichts
影響因子A linear integral equation is an equation of the form XEX. (1) 2a(x)cp(x) - Ix k(x, y)cp(y)dv(y) = f(x), Here (X, v) is a measure space with a-finite measure v, 2 is a complex parameter, and a, k, f are given (complex-valued) functions, which are referred to as the coefficient, the kernel, and the free term (or the right-hand side) of equation (1), respectively. The problem consists in determining the parameter 2 and the unknown function cp such that equation (1) is satisfied for almost all x E X (or even for all x E X if, for instance, the integral is understood in the sense of Riemann). In the case f = 0, the equation (1) is called homogeneous, otherwise it is called inhomogeneous. If a and k are matrix functions and, accordingly, cp and f are vector-valued functions, then (1) is referred to as a system of integral equations. Integral equations of the form (1) arise in connection with many boundary value and eigenvalue problems of mathematical physics. Three types of linear integralequations are distinguished: If 2 = 0, then (1) is called an equation of the first kind; if 2a(x) i= 0 for all x E X, then (1) is termed an equation of the second kind; and finally, if a vanishes on so
Pindex Book 1991
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書目名稱Analysis IV影響因子(影響力)




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0938-0396 en (1) is called an equation of the first kind; if 2a(x) i= 0 for all x E X, then (1) is termed an equation of the second kind; and finally, if a vanishes on so978-3-642-63491-8978-3-642-58175-5Series ISSN 0938-0396
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Linear Integral Equations,ed) functions, which are referred to as the ., the ., and the . (or the .) of equation (1), respectively. The problem consists in determining the parameter . and the unknown function . such that equation (1) is satisfied for almost all . ∈ . (or even for all x ∈ . if, for instance, the integral is u
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https://doi.org/10.1007/978-3-642-58175-5Integralgleichungen; Nichtstetige Randintegrale; Potential theory; Potentialtheorie; Randintegraltheorie
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978-3-642-63491-8Springer-Verlag Berlin Heidelberg 1991
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Encyclopaedia of Mathematical Scienceshttp://image.papertrans.cn/a/image/156140.jpg
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