Built on

A. Jevicki and B. Sakita, The Quantum Collective Field Method and Its Application to the Planar Limit
1981
Earlier work this paper cites.
P. Breitenlohner and D. Z. Freedman, Positive Energy in anti-De Sitter Backgrounds and Gauged Extended Supergravity
1982
Earlier work this paper cites.
C. Teitelboim, Gravitation and Hamiltonian Structure in Two Space-Time Dimensions
1983
Earlier work this paper cites.
R. Jackiw in " Quantum Theory of Gravity
1984
Earlier work this paper cites.
S. Sachdev and J. Ye, Gapless spin fluid ground state in a random, quantum Heisenberg magnet
1993
Earlier work this paper cites.
I. R. Klebanov and A. M. Polyakov, AdS dual of the critical O(N) vector model , Phys. Lett. B 550
2002
Earlier work this paper cites.
S. R. Das and A. Jevicki, Large N collective fields and holography
2003
Earlier work this paper cites.
S. Sachdev, Holographic metals and the fractionalized Fermi liquid
Original
2010
Earlier work this paper cites.
R. d. M. Koch, A. Jevicki, K. Jin and J. P. Rodrigues, A d S 4 / C F T 3 AdS_{4}/CFT_{3} Construction from Collective Fields
Original
2011
Earlier work this paper cites.
A. Kitaev, “Hidden Correlations in the Hawking Radiation and Thermal Noise,” talk given at Fundamental Physics Prize Symposium, Nov. 10, 2014
2014
Earlier work this paper cites.
S. H. Shenker and D. Stanford, Black holes and the butterfly effect
Original
2014
Earlier work this paper cites.
S. Leichenauer, Disrupting Entanglement of Black Holes
Original
2014
Earlier work this paper cites.
A. Jevicki, K. Jin and J. Yoon, 1/N and loop corrections in higher spin AdS 4 /CFT 3 duality
Original
2014
Earlier work this paper cites.
A. Kitaev, “A simple model of quantum holography,” KITP strings seminar and Entanglement 2015 program
2015
Earlier work this paper cites.
S. Sachdev, Bekenstein-Hawking Entropy and Strange Metals , Phys. Rev. X 5
Original
2015
Earlier work this paper cites.

Similar

S. H. Shenker and D. Stanford, Stringy effects in scrambling
Original
2015
Cited alongside, same era.
J. Maldacena, S. H. Shenker and D. Stanford, A bound on chaos
Original
2015
Cited alongside, same era.
J. Polchinski, Chaos in the black hole S-matrix
Original
2015
Cited alongside, same era.
R. de Mello Koch, A. Jevicki, J. P. Rodrigues and J. Yoon, Holography as a Gauge Phenomenon in Higher Spin Duality
Original
2015
Cited alongside, same era.
R. d. M. Koch, A. Jevicki, J. P. Rodrigues and J. Yoon, Canonical Formulation of O ⁡ ( N ) O(N) Vector/Higher Spin Correspondence
Original

Then

J. Engelsöy, T. G. Mertens and H. Verlinde, An investigation of AdS 2
Original
2016
Later among the works it cites.
D. Stanford and E. Witten, Fermionic Localization of the Schwarzian Theory
Original
2017
Closest in time.
T. G. Mertens, G. J. Turiaci and H. L. Verlinde, Solving the Schwarzian via the Conformal Bootstrap
Original
2017
Closest in time.
S. R. Das, A. Jevicki and K. Suzuki, Three Dimensional View of the SYK/AdS Duality
Original
2017
Closest in time.
M. Berkooz, P. Narayan, M. Rozali and J. Simï¿œn, Higher Dimensional Generalizations of the SYK Model
Original

Beyond the bibliography

alphaXiv searches the wider corpus for related work and actual follow-ups.

Open on alphaXiv

alphaXiv is searching for related work…

Reading the bibliography…

2017

Three Dimensional View of Arbitrary $q$ SYK models

Das, Sumit R., Ghosh, Animik, Jevicki, Antal et al.

Understand

In \url{arXiv:1704.07208} it was shown that the spectrum and bilocal propagator of SYK model with four fermion interactions can be realized as a three dimensional model in $AdS_2 \times S^1/Z_2$ with nontrivial boundary conditions in the additional dimension.

In this paper we show that a similar picture holds for generalizations of the SYK model with $q$-fermion interactions.
The 3D realization is now given on a space whose metric is conformal to $AdS_2 \times S^1/Z_2$ and is subject to a non-trivial potential in addition to a delta function at the center of the interval.
It is shown that a Horava-Witten compactification reproduces the exact SYK spectrum and a non-standard propagator between points which lie at the center of the interval exactly agrees with the bilocal propagator.