2017
DOI: 10.1007/s10711-017-0260-y
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The pressure metric on the Margulis multiverse

Abstract: This paper defines the pressure metric on the Moduli space of Margulis spacetimes without cusps and shows that it is positive definite on the constant entropy sections. It also demonstrates an identity regarding the variation of the cross-ratios.Date: September 12, 2018.

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Cited by 7 publications
(13 citation statements)
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References 51 publications
(129 reference statements)
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“…In this article we define affine crossratios for any four mutually transverse affine null planes in R 2n−1 and in Propositions 2.3.2 and 2.3.1 we show how they are intimately related with Margulis invariants. Similar results in the case of dimension three were found by Charette-Drumm in [CD04] and by Ghosh in [Gho17b]. Moreover, in Proposition 2.4.2, we also provide nice algebraic expressions for the linear counterparts, in SO 0 (n, n), of these affine crossratios.…”
Section: Introductionsupporting
confidence: 84%
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“…In this article we define affine crossratios for any four mutually transverse affine null planes in R 2n−1 and in Propositions 2.3.2 and 2.3.1 we show how they are intimately related with Margulis invariants. Similar results in the case of dimension three were found by Charette-Drumm in [CD04] and by Ghosh in [Gho17b]. Moreover, in Proposition 2.4.2, we also provide nice algebraic expressions for the linear counterparts, in SO 0 (n, n), of these affine crossratios.…”
Section: Introductionsupporting
confidence: 84%
“…We have also proved in Proposition 2.3.5 similar results regarding Margulis invariants. These expressions in the case of dimension three was already known by works of Charette-Drumm [CD04] and Ghosh [Gho17b].…”
Section: Introductionmentioning
confidence: 71%
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“…Ghosh [32] used work of Goldman, Labourie and Margulis [34,35] to interpret holonomy maps of Margulis space times (without cusps) as "Anosov representations" into the (non-semisimple) Lie group Aff(R 3 ) of affine automorphisms of R 3 . Ghosh [33] was then able to adapt the techniques of [17] to produce a pressure form on the analytic manifold M of (conjugacy classes of) holonomy maps of Margulis space times of fixed rank (with no cusps). This pressure form is an analytic Riemannian metric on the slice M k of M consisting of holonomy maps with entropy k (see Ghosh [33, Thm.…”
Section: Generalizations and Consequencesmentioning
confidence: 99%