The space of n-point correlation functions, for all possible time-orderings of operators, can be computed by a non-trivial path integral contour, which depends on how many time-ordering violations are present in the correlator. These contours, which have come to be known as timefolds, or out-of-time-order (OTO) contours, are a natural generalization of the Schwinger-Keldysh contour (which computes singly out-of-time-ordered correlation functions). We provide a detailed discussion of such higher OTO functional integrals, explaining their general structure, and the myriad ways in which a particular correlation function may be encoded in such contours. Our discussion may be seen as a natural generalization of the Schwinger-Keldysh formalism to higher OTO correlation functions. We provide explicit illustration for low point correlators (n=2,3,4) to exemplify the general statements.
Cited by 3
Arnab Kundu, Steady States, Thermal Physics, and Holography
Advances in High Energy Physics 2019, 1 (2019) [Crossref]
Soumyadeep Chaudhuri et al., Spectral representation of thermal OTO correlators
J. High Energ. Phys. 2019, 18 (2019) [Crossref]
Chi-Ming Chang et al., Spinning constraints on chaotic large c CFTs
J. High Energ. Phys. 2019, 68 (2019) [Crossref]
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- 1 University of British Columbia [UBC]
- 2 International Centre for Theoretical Sciences [ICTS-TIFR]
- 3 University of California, Davis [UCD]