Non-Schlesinger isomonodromic deformations of Fuchsian systems and middle convolution (Q2339262)
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| Language | Label | Description | Also known as |
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| English | Non-Schlesinger isomonodromic deformations of Fuchsian systems and middle convolution |
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Non-Schlesinger isomonodromic deformations of Fuchsian systems and middle convolution (English)
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31 March 2015
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The paper deals with the problem of constructing isomonodromy families of Fuchsian systems of the form \[ \frac{dy}{dz}=\left( \sum\limits_{i=1}^{n}{\frac{{{A}_{i}}(a)}{z-{{a}_{i}}}} \right)y,\quad \sum\limits_{i=1}^{n}{{{A}_{i}}(a)}=-{{A}_{n+1}}(a), \] where \(a=({{a}_{1}},\ldots ,{{a}_{n}})\) is a parameter and \({{A_i}(a)}\) is a matrix dependent on \(a\). Currently, there are few explicit examples of such families. The authors propose to build a new family from known one by the middle convolution method. They construct from a resonant family of order 2, using the middle convolution method, a new resonant family of order 5. Also in the paper an example is considered, when under this transformation the resonance disappears. Note that since the family is Fuchsian, all systems have the same Galois group. In this case, for constructing the isomonodromy family one can not considers equations of deformations of Schlesinger type, and use the results of \textit{J. Kovacic} [Ann. Math. (2) 89, 583--608 (1969; Zbl 0188.33801); Ann. Math. (2) 93, 269--284 (1971; Zbl 0214.06004)] on the inverse problem of differential Galois theory (see, for example, \textit{N. V. Grigorenko} [Ukr. Mat. Zh. 59, No. 8, 1131--1134 (2007); translation in Ukr. Math. J. 59, No. 8, 1253--1257 (2007; Zbl 1138.34042)]).
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middle convolution
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isomonodromic deformation
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non-Schlesinger isomonodromic deformation
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inverse problem
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differential Galois theory
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