39 research outputs found

    SYK-like Tensor Models on the Lattice

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    We study large NN tensor models on the lattice without disorder. We introduce techniques which can be applied to a wide class of models, and illustrate it by studying some specific rank-3 tensor models. In particular, we study Klebanov-Tarnopolsky model on lattice, Gurau-Witten model (by treating it as a tensor model on four sites) and also a new model which interpolates between these two models. In each model, we evaluate various four point functions at large NN and strong coupling, and discuss their spectrum and long time behaviors. We find similarities as well as differences from SYK model. We also generalize our analysis to rank-DD tensor models where we obtain analogous results as D=3D=3 case for the four point functions which we computed. For D>5D>5, we are able to compute the next-to-subleading 1N{1 \over N} corrections for a specific four point function.Comment: 46 pages, 29 figures; v2:typos corrected, reference added; v3:minor revisions, to be published in JHE

    Chiral 2D "Strange Metals" from N = 4 SYM

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    Familiar field theories may contain closed subsectors made out of only fermions, which can be used to explore new and unusual phases of matter in lower dimensions. We focus on the fermionic su(1,1) sector in N=4 SYM and on its ground states, which are Fermi surface states/operators. By computing their spectrum to order (gYM2N)2(g_{YM}^2 N)^2, we argue that fluctuations around this fermi surface, within the sector and in the limit kFk_F\rightarrow\infty, are governed by a chiral 1+1 dimensional sector of the "strange metal" coset SU(N)NSU(N)N/SU(N)2NSU(N)_N \otimes SU(N)_N/SU(N)_{2N}. On the gravity side, the conjectured dual configuration is an S=0S=0 degeneration of a rotating black hole. On general grounds we expect that the near horizon excitations of (S=0,Ω=1,J)(S=0,\Omega=1,J\rightarrow\infty) degenerations of black holes will be governed by a chiral sector of a 1+1 CFT.Comment: 44 page

    On monopole operators in supersymmetric Chern-Simons-matter theories

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    We discuss monopole operators in U(Nc)U(N_c) Chern-Simons-matter theories in three space-time dimensions. We mention an apparent problem in the matching of such operators in dualities between non-supersymmetric theories, and suggest a possible resolution. A similar apparent problem exists in the mapping of chiral monopole operators in theories with N=2{\cal N}=2 supersymmetry. We show that in many theories the lowest naive chiral monopole operator is actually not chiral, and we find the lowest monopole operator that is actually chiral in these theories. It turns out that there are several different forms of this operator, depending on the number of colors, the number of flavours, and the Chern-Simons level. Since we use the supersymmetric index to find the lowest chiral monopoles, our results for these monopoles are guaranteed to be invariant under the dualities in supersymmetric theories. The theories we discuss are believed to be dual in the 't~Hooft large NcN_c limit to classical high-spin gravity theories. We argue that these theories (supersymmetric or not) should not have classical solutions charged under the U(1)U(1) gauge field in the high-spin multiplet.Comment: 39 pages. v2: fixed typo

    Gravitational Edge Mode in Asymptotically AdS2_2: JT Gravity Revisited

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    We study the gravitational edge mode of the Jackiw-Teitelboim (JT) gravity and the constrained sl(2,R)sl(2,\mathbb{R}) BF theory for the asymptotically AdS2_2. We revisit the derivation of the Schwarzian theory from the wiggling boundary as an action for the gravitational edge mode. We present an alternative description for the gravitational edge mode from the metric fluctuation with the fixed boundary, which is also known as the would-be gauge mode in the gravity. We clarify the relation between the wiggling boundary and the would-be gauge mode. We demonstrate a natural top-down derivation of PSL(2,R)PSL(2,\mathbb{R}) gauging and the path integral measure of the Schwarzian theory. In the constrained sl(2,R)sl(2,\mathbb{R}) BF theory, we develop a method for incorporating the gravitational edge mode in the BF theory. In this BF theory coupled to the edge mode, we derive the Schwarzian theory with PSL(2,R)PSL(2,\mathbb{R}) gauging. We show that the Haar measure for the Iwasawa decomposition of PSL(2,R)PSL(2,\mathbb{R}) leads to the path integral measure.Comment: 32 pages, 6 figure

    Thermal out-of-time-order correlators, KMS relations, and spectral functions

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    We describe general features of thermal correlation functions in quantum systems, with specific focus on the fluctuation-dissipation type relations implied by the KMS condition. These end up relating correlation functions with different time ordering and thus should naturally be viewed in the larger context of out-of-time-ordered (OTO) observables. In particular, eschewing the standard formulation of KMS relations where thermal periodicity is combined with time-reversal to stay within the purview of Schwinger-Keldysh functional integrals, we show that there is a natural way to phrase them directly in terms of OTO correlators. We use these observations to construct a natural causal basis for thermal n-point functions in terms of fully nested commutators. We provide several general results which can be inferred from cyclic orbits of permutations, and exemplify the abstract results using a quantum oscillator as an explicit example.Comment: 36 pages + appendices. v2: minor changes + refs added. v3: minor changes, published versio

    Quantum groups, non-commutative AdS2AdS_2, and chords in the double-scaled SYK model

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    We study the double-scaling limit of SYK (DS-SYK) model and elucidate the underlying quantum group symmetry. The DS-SYK model is characterized by a parameter qq, and in the q1q\rightarrow 1 and low-energy limit it goes over to the familiar Schwarzian theory. We relate the chord and transfer-matrix picture to the motion of a ``boundary particle" on the Euclidean Poincar{\'e} disk, which underlies the single-sided Schwarzian model. AdS2AdS_2 carries an action of sl(2,R)su(1,1)\mathfrak{s}\mathfrak{l}(2,{\mathbb R}) \simeq \mathfrak{s}\mathfrak{u}(1,1), and we argue that the symmetry of the full DS-SYK model is a certain qq-deformation of the latter, namely Uq(su(1,1))\mathcal{U}_{\sqrt q}(\mathfrak{s}\mathfrak{u}(1,1)). We do this by obtaining the effective Hamiltonian of the DS-SYK as a (reduction of) particle moving on a lattice deformation of AdS2AdS_2, which has this Uq(su(1,1))\mathcal{U}_{\sqrt q}(\mathfrak{s}\mathfrak{u}(1,1)) algebra as its symmetry. We also exhibit the connection to non-commutative geometry of qq-homogeneous spaces, by obtaining the effective Hamiltonian of the DS-SYK as a (reduction of) particle moving on a non-commutative deformation of AdS3AdS_3. There are families of possibly distinct qq-deformed AdS2AdS_2 spaces, and we point out which are relevant for the DS-SYK model.Comment: 70 pages, 6 figure

    Schwinger-Keldysh superspace in quantum mechanics

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    We examine, in a quantum mechanical setting, the Hilbert space representation of the BRST symmetry associated with Schwinger-Keldysh path integrals. This structure had been postulated to encode important constraints on influence functionals in coarse-grained systems with dissipation, or in open quantum systems. Operationally, this entails uplifting the standard Schwinger-Keldysh two-copy formalism into superspace by appending BRST ghost degrees of freedom. These statements were previously argued at the level of the correlation functions. We provide herein a complementary perspective by working out the Hilbert space structure explicitly. Our analysis clarifies two crucial issues not evident in earlier works: firstly, certain background ghost insertions necessary to reproduce the correct Schwinger-Keldysh correlators arise naturally. Secondly, the Schwinger-Keldysh difference operators are systematically dressed by the ghost bilinears, which turn out to be necessary to give rise to a consistent operator algebra. We also elaborate on the structure of the final state (which is BRST closed) and the future boundary condition of the ghost fields.Comment: 30 page
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