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Title: Toward a holographic theory for general spacetimes

Authors:
; ; ;
Publication Date:
Sponsoring Org.:
USDOE
OSTI Identifier:
1349704
Grant/Contract Number:
AC02-05CH11231; SC0011702
Resource Type:
Journal Article: Publisher's Accepted Manuscript
Journal Name:
Physical Review D
Additional Journal Information:
Journal Volume: 95; Journal Issue: 8; Related Information: CHORUS Timestamp: 2017-04-03 22:15:51; Journal ID: ISSN 2470-0010
Publisher:
American Physical Society
Country of Publication:
United States
Language:
English

Citation Formats

Nomura, Yasunori, Salzetta, Nico, Sanches, Fabio, and Weinberg, Sean J. Toward a holographic theory for general spacetimes. United States: N. p., 2017. Web. doi:10.1103/PhysRevD.95.086002.
Nomura, Yasunori, Salzetta, Nico, Sanches, Fabio, & Weinberg, Sean J. Toward a holographic theory for general spacetimes. United States. doi:10.1103/PhysRevD.95.086002.
Nomura, Yasunori, Salzetta, Nico, Sanches, Fabio, and Weinberg, Sean J. Mon . "Toward a holographic theory for general spacetimes". United States. doi:10.1103/PhysRevD.95.086002.
@article{osti_1349704,
title = {Toward a holographic theory for general spacetimes},
author = {Nomura, Yasunori and Salzetta, Nico and Sanches, Fabio and Weinberg, Sean J.},
abstractNote = {},
doi = {10.1103/PhysRevD.95.086002},
journal = {Physical Review D},
number = 8,
volume = 95,
place = {United States},
year = {Mon Apr 03 00:00:00 EDT 2017},
month = {Mon Apr 03 00:00:00 EDT 2017}
}

Journal Article:
Free Publicly Available Full Text
Publisher's Version of Record at 10.1103/PhysRevD.95.086002

Citation Metrics:
Cited by: 5works
Citation information provided by
Web of Science

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  • Cited by 7
  • The butterfly velocity characterizes the spread of correlations in a quantum system. Recent work has provided a method of calculating the butterfly velocity of a class of boundary operators using holographic duality. Utilizing this and a presumed extension of the canonical holographic correspondence of AdS/CFT, we investigate the butterfly velocities of operators with bulk duals living in general spacetimes. We analyze some ubiquitous issues in calculating butterfly velocities using the bulk effective theory, and then extend the previously proposed method to include operators in entanglement shadows. Here in this paper, we explicitly compute butterfly velocities for bulk local operators inmore » the holographic theory of flat Friedmann-Robertson-Walker spacetimes and find a universal scaling behavior for the spread of operators in the boundary theory, independent of dimension and fluid components. This result may suggest that a Lifshitz field theory with z = 4 is the appropriate holographic dual for these spacetimes.« less
  • We describe probes of anti{endash}de Sitter spacetimes in terms of conformal field theories on the AdS boundary. Our basic tool is a formula that relates bulk and boundary states{emdash}classical bulk field configurations are dual to expectation values of operators on the boundary. At the quantum level we relate the operator expansions of bulk and boundary fields. Using our methods, we discuss the CFT description of local bulk probes including normalizable wave packets, fundamental and D-strings, and D-instantons. Radial motions of probes in the bulk spacetime are related to motions in scale on the boundary, demonstrating a scale-radius duality. We discussmore » the implications of these results for the holographic description of black hole horizons in the boundary field theory. {copyright} {ital 1999} {ital The American Physical Society}« less
  • We prove a c-theorem for holographic renormalization group flows in a Schrodinger spacetime that demonstrates that the effective radius L(r) monotonically decreases from the UV to the IR, where r is the bulk radial coordinate. This result assumes that the bulk matter satisfies the null energy condition, but holds regardless of the value of the critical exponent z. We also construct several numerical examples in a model where the Schrodinger background is realized by a massive vector coupled to a real scalar. Finally, the full Schrodinger group is realized when z = 2, and in this case it is possiblemore » to construct solutions with constant effective z(r) = 2 along the entire flow.« less