13 research outputs found

    Double-scaled SYK and de Sitter Holography

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    We propose a new model of low dimensional de Sitter holography in the form of a pair of double-scaled SYK models at infinite temperature coupled via an equal energy constraint HL=HRH_L=H_R. As a test of the duality, we compute the two-point function between two dressed SYK operators OΞ”{\cal O}_\Delta that preserve the constraint. We find that in the large NN limit, the two-point function precisely matches with the Green's function of a massive scalar field of mass squared m2=4Ξ”(1βˆ’Ξ”)m^2 = 4\Delta(1-\Delta) in a 3D de Sitter space-time with radius RdS/GN=4Ο€N/p2R_{\text{dS}}/G_N = 4\pi N/p^2. In this correspondence, the SYK time is identified with the proper time difference between the two operators. We introduce a candidate gravity dual of the doubled SYK model given by a JT/de Sitter gravity model obtained via a circle reduction from 3D Einstein-de Sitter gravity. We comment on the physical meaning of the finite de Sitter temperature and entropy.Comment: 26 pages, 4 figure

    Towards a full solution of the large N double-scaled SYK model

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    We compute the exact, all energy scale, 4-point function of the large NN double-scaled SYK model, by using only combinatorial tools and relating the correlation functions to sums over chord diagrams. We apply the result to obtain corrections to the maximal Lyapunov exponent at low temperatures. We present the rules for the non-perturbative diagrammatic description of correlation functions of the entire model. The latter indicate that the model can be solved by a reduction of a quantum deformation of SL(2)(2), that generalizes the Schwarzian to the complete range of energies.Comment: 52+28 pages, 14 figures; v2: references revised, typos corrected, changed normalization of SL(2)_q 6j symbo

    A supersymmetric SYK model with a curious low energy behavior

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    We consider N\mathcal{N} = 2, 4 supersymmetric SYK models that have a peculiar low energy behavior, with the entropy going like S=S0+(constant)TaS = S_{0} + \text{(constant)}T^{a}, where a≠1a \neq 1. The large NN equations for these models are a generalization of equations that have been previously studied as an unjustified truncation of the planar diagrams describing the BFSS matrix quantum mechanics or other related matrix models. Here we reanalyze these equations in order to better understand the low energy physics of these models. We find that the scalar fields develop large expectation values which explore the low energy valleys in the potential. The low energy physics is dominated by quadratic fluctuations around these values. These models were previously conjectured to have a spin glass phase. We did not find any evidence for this phase by using the usual diagnostics, such as searching for replica symmetry breaking solutions

    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 qβ†’1q\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

    Multi-trace Correlators in the SYK Model and Non-geometric Wormholes

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    We consider multi-energy level distributions in the SYK model, and in particular, the role of global fluctuations in the density of states of the SYK model. The connected contributions to the moments of the density of states go to zero as Nβ†’βˆžN \to \infty, however, they are much larger than the standard RMT correlations. We provide a diagrammatic description of the leading behavior of these connected moments, showing that the dominant diagrams are given by 1PI cactus graphs, and derive a vector model of the couplings which reproduces these results. We generalize these results to the first subleading corrections, and to fluctuations of correlation functions. In either case, the new set of correlations between traces (i.e. between boundaries) are not associated with, and are much larger than, the ones given by topological wormholes. The connected contributions that we discuss are the beginning of an infinite series of terms, associated with more and more information about the ensemble of couplings, which hints towards the dual of a single realization. In particular, we suggest that incorporating them in the gravity description requires the introduction of new, lighter and lighter, fields in the bulk with fluctuating boundary couplings.Comment: 81 pages, 23 figures. V2: added short discussion on the modified dip time, and corrected minor typo

    Dualities between fermionic theories and the Potts model

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    Abstract We show that a large class of fermionic theories are dual to a q β†’ 0 limit of the Potts model in the presence of a magnetic field. These can be described using a statistical model of random forests on a graph, generalizing the (unrooted) random forest description of the Potts model with only nearest neighbor interactions. We then apply this to find a statistical description of a recently introduced family of OSp(1|2M) invariant field theories that provide a UV completion to sigma models with the same symmetry
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