On an integral equation of the form \(u(x)= F(x)+ \int G(x,\xi)u_ +^{(n-2)/2}(\xi)d\xi/ \int u_ +^{(n-2)/2}(\xi)d\xi\) for \(n=2\) and \(n=3\) (Q1893649)
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scientific article; zbMATH DE number 771993
| Language | Label | Description | Also known as |
|---|---|---|---|
| English | On an integral equation of the form \(u(x)= F(x)+ \int G(x,\xi)u_ +^{(n-2)/2}(\xi)d\xi/ \int u_ +^{(n-2)/2}(\xi)d\xi\) for \(n=2\) and \(n=3\) |
scientific article; zbMATH DE number 771993 |
Statements
On an integral equation of the form \(u(x)= F(x)+ \int G(x,\xi)u_ +^{(n-2)/2}(\xi)d\xi/ \int u_ +^{(n-2)/2}(\xi)d\xi\) for \(n=2\) and \(n=3\) (English)
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10 July 1995
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The integral equation \[ u(x)= F(x)+ {\int_{u> 0} G(x, \xi) u^{(n- 2)/2}(\xi)d\xi\over \int_{u> 0} u^{(n- 2)/2} (\xi)d\xi} \] is deduced heuristically, where \(x\in \mathbb{R}^n\), \(\xi\in \mathbb{R}^n\), the function \(G(x, \xi)\) plays the role of the potential of the particle interaction, and the function \(F(x)\) the role of an external potential. The most frequent cases in physics are for \(n= 3\), when the attractive or repulsive potential is of the form \({\alpha\over r}\), where \(\alpha> 0\) is a physical constant, and \(r= \sqrt{(x_1- \xi_1)^2+ (x_2- \xi_2)^2+ (x_3- \xi_3)^2}\) is the distance between particles. Under some conditions, the existence and uniqueness of a continuous solution for the above integral equation are studied.
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integral equation
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potential
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particle interaction
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external potential
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existence
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uniqueness
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continuous solution
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