2020
DOI: 10.1214/19-aop1377
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The distribution of Gaussian multiplicative chaos on the unit interval

Abstract: We consider a sub-critical Gaussian multiplicative chaos (GMC) measure defined on the unit interval [0, 1] and prove an exact formula for the fractional moments of the total mass of this measure. Our formula includes the case where log-singularities (also called insertion points) are added in 0 and 1, the most general case predicted by the Selberg integral. The idea to perform this computation is to introduce certain auxiliary functions resembling holomorphic observables of conformal field theory that will be … Show more

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Cited by 18 publications
(27 citation statements)
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“…However, there is nothing obviously special about γ = √ 8/3 from either of the definitions of the LQG metric given in this paper (the limit of LFPP or the axiomatic definition). There has been a recent proliferation of exact formulas for quantities related to the γ -LQG area and boundary length measures for general γ ∈ (0, 2), proven using ideas from conformal field theory: see, e.g., [54,75,77]. In the special case when γ = √ 8/3, exact formulas for various quantities associated with the √ 8/3-LQG metric can be obtained using its connection to the Brownian surfaces.…”
Section: Additional Properties Of the Lqg Metricmentioning
confidence: 99%
“…However, there is nothing obviously special about γ = √ 8/3 from either of the definitions of the LQG metric given in this paper (the limit of LFPP or the axiomatic definition). There has been a recent proliferation of exact formulas for quantities related to the γ -LQG area and boundary length measures for general γ ∈ (0, 2), proven using ideas from conformal field theory: see, e.g., [54,75,77]. In the special case when γ = √ 8/3, exact formulas for various quantities associated with the √ 8/3-LQG metric can be obtained using its connection to the Brownian surfaces.…”
Section: Additional Properties Of the Lqg Metricmentioning
confidence: 99%
“…In the discrete setting, they compute the first few low moments (which agree with the first few explicit examples computed in Appendix A) and establish a connection to the KPP equation in the continuous setting. Additionally, it is natural to ask if the leading order coefficient ρ(k, β) for kβ 2 < 1 in (14) could take the form f (β) k Γ (1 − kβ 2 ) for some function f , in line with Fyodorov-Bouchaud [17] or Remy-Zhu [28] formulae for related problems in the same regime (see also (13)). Such a statement does not appear to hold here.…”
Section: Resultsmentioning
confidence: 96%
“…For example, ρ(2, β), σ(2, β), and τ (2, β) are given respectively by (27),(28), and (30). Although the k = 1 case exhibits no phase transition, we will write for ease of notationρ(1, β) ≡ σ (1, β) ≡ τ (1, β) = 1.…”
mentioning
confidence: 99%
“…The BPZ equations are essential for proving integrability of LCFT. They were used in the proof of the DOZZ-formula [14,15] for the 3-point function of LCFT on the sphere, and after this similar methods were used for obtaining integrability results for one dimensional GMC measures on the unit circle [19] and on the unit interval [20]. The unit circle computation was based on a boundary LCFT, which is defined in [11].…”
Section: 2mentioning
confidence: 99%