2017
DOI: 10.1093/imrn/rnw283
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Finite Braid group orbits in $\mathbf{Aff}\boldsymbol{(\mathbb{C})}$-character varieties of the punctured sphere

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Cited by 8 publications
(7 citation statements)
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“…A similar simplification holds for each inhomogeneous system (5). Note that N i=1 d b k,k+1 i (a) ≡ 0, and thus system (7) is equivalent to…”
Section: A Particular Case Of the Exponents And Solutions Via Periodsmentioning
confidence: 92%
See 1 more Smart Citation
“…A similar simplification holds for each inhomogeneous system (5). Note that N i=1 d b k,k+1 i (a) ≡ 0, and thus system (7) is equivalent to…”
Section: A Particular Case Of the Exponents And Solutions Via Periodsmentioning
confidence: 92%
“…With respect to this correspondence, in the case of a non-degenerate linear monodromy (that is, neither finite, nor dihedral, nor triangular), algebraic solutions were partially classified by K. Diarra [9] for an arbitrary M and by P. Calligaris, M. Mazzocco [4] for M = 2. For a non-abelian triangular linear monodromy, the classification of Schlesinger isomonodromic (2 × 2)families leading to algebraic solutions of Garnier systems, was done by G. Cousin, D. Moussard [7]. For a dihedral linear monodromy, there are families of algebraic solutions obtained by A. Girand [17], for M = 2 and by A. Komyo [28] for an arbitrary even M .…”
Section: Families Of Algebraic Solutions Of Garnier Systems: a Sphere...mentioning
confidence: 99%
“…The reader will find a more precise statement in [10]. Let us just mention in the first case the works of Girand [19] and Komyo [33] for deformations of equation ( 1) with dihedral monodromy, and Cousin and Moussard [13] in the reducible case. Deformations of equation ( 1) having a finite group are algebraic and provide an algebraic Garnier solution in a systematic way, but computations can be very tedious as it has been in the works of Boalch for the Painlevé case N = 1.…”
Section: Himentioning
confidence: 99%
“…(and a twist) to reduce the matrix A in the companion form (12): set F dx = γ and G = 0. One can further reduce (12), or accordingly (11), by gauge transformation (13) with F ≡ 1, or equivalently setting u := u/ exp( G); by this way, we can arrive to the unique SL-form ( 14)…”
Section: Monodromy and Stokes Matricesmentioning
confidence: 99%
“…We then apply this explicit description of the mapping class group action to the specific study of finite g,n -orbits on χ g,n (GL 2 C) that correspond to reducible representations. For g = 0, this study has been completely carried out in [8]. In this special case, the study can be reduced to linear dynamics.…”
Section: B Dynamical Study Of Finite Orbits In the Reducible Rank 2 Casementioning
confidence: 99%