2019
DOI: 10.1215/00127094-2018-0059
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Isomonodromy deformations at an irregular singularity with coalescing eigenvalues

Abstract: We consider an n × n linear system of ODEs with an irregular singularity of Poincaré rank 1 at z = ∞, holomorphically depending on parameter t within a polydisc in C n centred at t = 0. The eigenvalues of the leading matrix at z = ∞ coalesce along a locus ∆ contained in the polydisc, passing through t = 0. Namely, z = ∞ is a resonant irregular singularity for t ∈ ∆. We analyse the case when the leading matrix remains diagonalisable at ∆. We discuss the existence of fundamental matrix solutions, their asymptoti… Show more

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Cited by 30 publications
(178 citation statements)
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“…In a series of papers[5][6][7], Cotti, Dubrovin, and Guzzetti study semisimple Frobenius structures with coalescing eigenvalues. It would be very interesting to clarify the relation between Conjecture 1.12 and the Stokes phenomenon of the Dubrovin's connection in quantum cohomology studied in loc.…”
mentioning
confidence: 99%
“…In a series of papers[5][6][7], Cotti, Dubrovin, and Guzzetti study semisimple Frobenius structures with coalescing eigenvalues. It would be very interesting to clarify the relation between Conjecture 1.12 and the Stokes phenomenon of the Dubrovin's connection in quantum cohomology studied in loc.…”
mentioning
confidence: 99%
“…These notes partly touch the topics of my talk in Ann Arbor at the conference in memory of Andrei Kapaev, August 2017. They are a reworking of some of the main results of [11], concerning non-generic isomonodromy deformations of the differential system (2.1) below. The approach here is different from [11], since I will start from the point of view of Pfaffian systems.…”
Section: Introductionmentioning
confidence: 98%
“…They are a reworking of some of the main results of [11], concerning non-generic isomonodromy deformations of the differential system (2.1) below. The approach here is different from [11], since I will start from the point of view of Pfaffian systems. This allows to introduce the main theorem (Theorem 4.9 below) in a relatively simple way (provided we give for granted another result of [11] summarised in Theorem 4.7 below).…”
Section: Introductionmentioning
confidence: 98%
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