2021
DOI: 10.48550/arxiv.2111.04715
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Boundary timelike Liouville theory: bulk 1-point & boundary 2-point functions

Abstract: We consider timelike Liouville theory with FZZT-like boundary conditions. The bulk one-point and boundary two-point structure constants on a disk are derived using bootstrap. We find that these structure constants are not the analytic continuations of their spacelike counterparts.

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Cited by 3 publications
(4 citation statements)
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“…Alternatively, we could also consider deforming the contour of integration for τ 2 into the complexified τ 2 plane-this approach will invariably present further ambiguities. Given the divergences at higher genera for c m ⩾ 25, it is interesting to note that a potentially ultraviolet finite quantity independent of the normalisation of the path-integral is given by the ratio of the sphere path integral to the square of the disk partition function (this quantity was investigated in [35] for c m ≪ 1 and the disk partition function of timelike Liouville theory was studied in [36]). The general lesson is that much like for one-dimensional quantum gravity, the two-dimensional Euclidean path integral over compact manifolds needs to be regularised in a non-standard way.…”
Section: Dimension Twomentioning
confidence: 99%
“…Alternatively, we could also consider deforming the contour of integration for τ 2 into the complexified τ 2 plane-this approach will invariably present further ambiguities. Given the divergences at higher genera for c m ⩾ 25, it is interesting to note that a potentially ultraviolet finite quantity independent of the normalisation of the path-integral is given by the ratio of the sphere path integral to the square of the disk partition function (this quantity was investigated in [35] for c m ≪ 1 and the disk partition function of timelike Liouville theory was studied in [36]). The general lesson is that much like for one-dimensional quantum gravity, the two-dimensional Euclidean path integral over compact manifolds needs to be regularised in a non-standard way.…”
Section: Dimension Twomentioning
confidence: 99%
“…(15). In the case of LFT (with the correct background charge) such factor is instead m r=1 r −2 = (−1) −4m Γ −2 (m + 1); see the last factor in (33). In (15) the Γ-functions in the denominator combine with the overall factor Γ(−m−3)Γ(m+1) in the numerator, yielding…”
Section: Timelike Partition Functionmentioning
confidence: 99%
“…These results were extended in [31], where a computation at 3-loops was performed in a similar framework. More works along this line appeared recently: In [32], the semiclassical gravitational path integral was discussed in relation to random matrices, and in [33] the timelike LFT computation was performed in presence of boundaries. The latter work nicely shows how subtle the analytic continuation that connects the spacelike LFT to its timelike version can be.…”
Section: Introductionmentioning
confidence: 99%
“…These results were extended in [30], where a computation at 3-loops was performed in a similar framework. More works along this line appeared recently: in [31], the semiclassical gravitational path integral was discussed in relation to random matrices, and in [32] the timelike LFT computation was performed in presence of boundaries. The latter work nicely shows how subtle the analytic continuation that connects the spacelike LFT to its timelike version can be.…”
Section: Introductionmentioning
confidence: 99%