2022
DOI: 10.1007/s00208-021-02337-w
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On the monodromy of the deformed cubic oscillator

Abstract: We study a second-order linear differential equation known as the deformed cubic oscillator, whose isomonodromic deformations are controlled by the first Painlevé equation. We use the generalised monodromy map for this equation to give solutions to the Riemann-Hilbert problems of (Bridgeland in Invent Math 216(1):69–124, 2019) arising from the Donaldson-Thomas theory of the A$$_2$$ 2 quiver. These are the first known solution… Show more

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Cited by 7 publications
(17 citation statements)
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“…Thus the question as to whether the connection ∇ J is well-defined becomes an interesting one. Note that in the one example that has been computed in detail [18], the connection ∇ J is indeed well-defined, and turns out to be quite natural.…”
Section: Given a Symplectic ν-Pencil Hmentioning
confidence: 81%
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“…Thus the question as to whether the connection ∇ J is well-defined becomes an interesting one. Note that in the one example that has been computed in detail [18], the connection ∇ J is indeed well-defined, and turns out to be quite natural.…”
Section: Given a Symplectic ν-Pencil Hmentioning
confidence: 81%
“…Turning to the equation (62), note that the first term on the right-hand-side is the invariant vector field U = i z i • ∂/∂θ i on T # M,p corresponding to the value E p ∈ T M,p of the vector field (18). Exponentiating yields well-defined automorphisms exp(U/ǫ) of T # M,p given in coordinates by θ i → θ i + ǫ −1 z i .…”
Section: Preferred Co-ordinates and Stokes Datamentioning
confidence: 99%
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