2012
DOI: 10.5802/aif.2696
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Multiple Bernoulli series, an Euler-MacLaurin formula, and Wall crossings

Abstract: Using multiple Bernoulli series, we give a formula in the spirit of Euler-MacLaurin formula. We also give a wall crossing formula and a decomposition formula for multiple Bernoulli series. The study of these series is motivated by formulae of E. Witten for volumes of moduli spaces of flat bundles over a surface.

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Cited by 8 publications
(14 citation statements)
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“…[20]). In these examples, the twisted DuistermaatHeckman distributions are essentially Bernoulli series, and the formula (1) coincides with the decomposition formula in [8]. (These examples are closely related to Witten's formulas for intersection pairings on moduli spaces of flat connections on Riemann surfaces.)…”
Section: Introductionmentioning
confidence: 82%
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“…[20]). In these examples, the twisted DuistermaatHeckman distributions are essentially Bernoulli series, and the formula (1) coincides with the decomposition formula in [8]. (These examples are closely related to Witten's formulas for intersection pairings on moduli spaces of flat connections on Riemann surfaces.)…”
Section: Introductionmentioning
confidence: 82%
“…In this example the contribution from 0 vanishes, and the remaining terms in (1) are constant multiples (±1 relative to suitably normalized Lebesgue measure) of indicator functions for half-spaces (see Section 5 for further discussion). The formula (1) is related to the decomposition formula for Bernoulli series in [8]. Indeed, a collection of examples of Hamiltonian loop group spaces are moduli spaces of flat connections on a compact Riemann surface having at least 1 boundary component, with moment map given by pullback of the connection to the boundary (cf.…”
Section: Introductionmentioning
confidence: 99%
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“…In this case, s = 1, p = 0, q = 1, f = 3, |Z(SU(3))| = 3, hence, for g = 2, 2 s(2g−1) (f q) g−1 |Z(G)|(−1) (g−1)|Φ| = −3 2 . vol(SU(3), g = 2)(a) = −9 γ∈Preg e 2iπ a,γ Hα∈Φ (2iπ H α , γ ) 3 = −9 n 1 =0,n 2 =0,n 1 +n 2 =0 e 2iπ(n 1 a 1 +n 2 a 2 ) (2iπn 1 ) 3 (2iπn 2 ) 3 (2iπ(n 1 + n 2 )) 3 and we obtain vol(SU(3), g = 2)(a) = 1/40320(a 2 − 2a 1 )(a 2 − 1 + a 1 )(−1 + 2a 2 − a 1 )P 1 , a 1 ≤ a 2 1/40320(a 2 + 1 − 2a 1 )(2a 2 − a 1 )(a 2 − 1 + a 1 )P 2 , a 1 ≥ a 2…”
Section: Various Examples Of Volume Calculationsmentioning
confidence: 99%
“…In this example the contribution from 0 vanishes, and the remaining terms in (1) are constant multiples (±1 relative to suitably normalized Lebesgue measure) of indicator functions for half-spaces (see Section 5 for further discussion). The formula (1) is related to the decomposition formula for Bernoulli series in [8]. Indeed, a collection of examples of Hamiltonian loop group spaces are moduli spaces of flat connections on a compact Riemann surface having at least 1 boundary component, with moment map given by pullback of the connection to the boundary (cf.…”
Section: Introductionmentioning
confidence: 99%