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The talk argues that Jackiw–Teitelboim (JT) gravity on finite-size geometries can be defined with a conformal-gauge path integral. For flat JT on the disk, that path integral is a log-correlated boundary field plus a...
Unknown · 0:00
The talk argues that Jackiw–Teitelboim (JT) gravity on finite-size geometries can be defined with a conformal-gauge path integral. For flat JT on the disk, that path integral is a log-correlated boundary field plus a...
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