2015
DOI: 10.4310/mrl.2015.v22.n3.a12
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Nonabelian Hodge theory in positive characteristic via exponential twisting

Abstract: Let k be a perfect field of odd characteristic and X a smooth algebraic variety over k which is W 2 -liftable. We show that the exponent twisiting of the classical Cartier descent gives an equivalence of categories between the category of nilpotent Higgs sheaves of exponent ≤ p − 1 over X/k and the category of nilpotent flat sheaves of exponent ≤ p − 1 over X/k, and it is equivalent up to sign to the inverse Cartier and Cartier transforms for these nilpotent objects constructed in the nonabelian Hodge theory i… Show more

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Cited by 19 publications
(31 citation statements)
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“…When D = ∅, this was first proved in [OV,thm 2.8]. A simplified construction of the correspondence in the last case can be found in [LSZ2].…”
Section: Proof Of Theoremmentioning
confidence: 86%
“…When D = ∅, this was first proved in [OV,thm 2.8]. A simplified construction of the correspondence in the last case can be found in [LSZ2].…”
Section: Proof Of Theoremmentioning
confidence: 86%
“…In the work of [OV07], Ogus and Vologodsky established such a correspondence for nilpotent objects. More precisely, under the assumption that a lifting of X /S modulo p 2 exists, where X is the Frobenius twist of X, they construct a Cartier transform from the category of modules with flat connections nilpotent of exponent 1 ≤ p to the category of Higgs modules nilpotent of exponent ≤ p. There is an alternative approach to this result in [LSZ15]. A generalisation of this work to higher level arithmetic differential operators (in the sense of [Ber96]) is given in [GLQ10].…”
Section: Introductionmentioning
confidence: 99%
“…Let C −1 1 be the inverse Cartier transform of Ogus-Vologodsky from the category of nilpotent logarithmic Higgs module of exponent ≤ p − 1 to the category of nilpotent logarithmic flat module of exponent ≤ p − 1 with respect to the chosen W 2 -lifting (X 2 , D 2 ). We refer the reader to [LSZ0] for an elementary approach to the construction of the inverse Cartier/Cartier transform in the case D 1 = ∅ and the Appendix in a special log case. A Higgs-de Rham flow over X 1 is a diagram of the following form: where the initial term (E 0 , θ 0 ) is a nilpotent graded Higgs bundle with exponent ≤ p − 1; for i ≥ 0, F il i is a Hodge filtration on the flat bundle C −1 1 (E i , θ i ) of level ≤ p−1; for i ≥ 1, (E i , θ i ) is the graded Higgs bundle associated with the de Rham bundle (C −1 1 (E i−1 , θ i−1 ), F il i−1 ).…”
Section: Introductionmentioning
confidence: 99%