2022
DOI: 10.1007/jhep09(2022)126
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2D quantum gravity partition function on the fluctuating sphere

Abstract: Motivated by recent works on the connection between 2D quantum gravity and timelike Liouville theory, we revisit the latter and clarify some aspects of the computation of its partition function: we present a detailed computation of the Liouville partition function on the fluctuating sphere at finite values of the central charge. The results for both the spacelike theory and the timelike theory are given, and their properties analyzed. We discuss the derivation of the partition function from the DOZZ formula, i… Show more

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Cited by 6 publications
(4 citation statements)
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“…Some of these contributions can be interpreted as entanglement entropy for gravitational edge modes [103,104]. Similar expressions have been studied in 𝑑 = 3, where there exists an all-loop calculation [28,105,106] and in 𝑑 = 2, where a non-perturbative formula in timelike Liouville theory has been conjectured [107][108][109][110][111][112][113].…”
Section: Static Patch Holography and Timelike Boundariesmentioning
confidence: 67%
“…Some of these contributions can be interpreted as entanglement entropy for gravitational edge modes [103,104]. Similar expressions have been studied in 𝑑 = 3, where there exists an all-loop calculation [28,105,106] and in 𝑑 = 2, where a non-perturbative formula in timelike Liouville theory has been conjectured [107][108][109][110][111][112][113].…”
Section: Static Patch Holography and Timelike Boundariesmentioning
confidence: 67%
“…The fact that the s insertions are integrated means that they are hard sources that constitute the wall, and so they are integrated over the whole non-compact direction X 0 . According to this, the prefactor Γ(−s) in (22) has the same interpretation as the one given in [8]; it is the factor associated to the poles of resonant correlators with a definite number of tachyon insertions.…”
Section: Interpretation Of (22)mentioning
confidence: 85%
“…In particular, the limiting procedure connecting the three-point function to the two-point function is puzzling [11]. The special features of the timelike three-point function were discussed by many authors, and notably by Harlow, Maltz, and Witten in [10]; see also [15]- [22] and references therein and thereof. Our computation, however, only relies on the expression for the two-point function, for which no special features are expected to appear and the result was expected to yield the correct two-point function as shown.…”
Section: Discussionmentioning
confidence: 99%
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