2008
DOI: 10.1007/s10440-008-9189-3
|View full text |Cite
|
Sign up to set email alerts
|

On the Painlevé Property of Isomonodromic Deformations of Fuchsian Systems

Abstract: We give a review of the modern theory of isomonodromic deformations of Fuchsian systems discussing both classical and modern results, such as a general form of the isomonodromic deformations of Fuchsian systems, their differences from the classical Schlesinger deformations, the Fuchsian system moduli space structure and the geometric meaning of new degrees of freedom appeared in a non-Schlesinger case. Using this we illustrate some general relations between such concepts as integrability, isomonodromy and Pain… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1

Citation Types

0
2
0
1

Year Published

2008
2008
2019
2019

Publication Types

Select...
3
2

Relationship

0
5

Authors

Journals

citations
Cited by 5 publications
(3 citation statements)
references
References 8 publications
0
2
0
1
Order By: Relevance
“…That is, we consider the member of isomonodromy family of the BHC (1.3) at the exceptional point z = 0, y = 0, z/y = λ. Since all the isomonodromy integral curves in the yz−plane pass through the exceptional line of the blow up (z, z/y) → (z, y) (see [39]), no generality is lost.…”
Section:  mentioning
confidence: 99%
“…That is, we consider the member of isomonodromy family of the BHC (1.3) at the exceptional point z = 0, y = 0, z/y = λ. Since all the isomonodromy integral curves in the yz−plane pass through the exceptional line of the blow up (z, z/y) → (z, y) (see [39]), no generality is lost.…”
Section:  mentioning
confidence: 99%
“…The system of PDEs dY = ωY is over-determined in general and does not have any local solutions. However, the flatness condition dω = ω ∧ ω guarantees the existence of local solutions of dY = ωY (see [24]). If one chooses a convenient basis so that A 3 is diagonal, such a flatness condition implies that X(t), the zero locus of the (1,2) entry of ω, satisfies the usual Painlevé VI equation [16, §3], [30, §2].…”
Section: The Correspondence To the Elliptic Painlevé VI Equationmentioning
confidence: 99%
“…Тем не менее можно показать, что пространство M * a естественным образом расслаивается на листы, для каждого из которых отображение RH a корректно определено (хотя и не на всем пространстве M a ; подробнее см. [60]). …”
unclassified