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Holographic Fisher Information Metric in Schr\"odinger Spacetime

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arxiv 2009.01123 v4 pith:ZVKMZGMK submitted 2020-09-02 hep-th

Holographic Fisher Information Metric in Schr\"odinger Spacetime

classification hep-th
keywords informationtheoryholographicmetricboundaryfisherspacetimefield
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved
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In this paper we study the Fisher information metric on the space of the coupling constants on both sides of the duality between non-relativistic dipole field theories and string theory in Schr\"odinger spacetime. We consider the following setup. In the gauge theory side one can deform a given conformal field theory by a proper scalar operator and compute the quantum information metric via the two-point correlation function between two such operators. On the string side the deformation corresponds to a scalar field probing the background. In the large $N$ limit of the theory the probing can be done without backreaction on the original spacetime, thus one can construct a perturbative scheme for the calculation of the dual holographic Fisher information metric as shown by \cite{Trivella:2016brw}. Considering the asymptotic behaviour of the holographic Fisher information metric close to the boundary of the Schr\"odinger spacetime we show that its divergence structure exactly matches its dual quantum counterpart up to the leading order, thus extending the holographic setup up to the non-relativistic case. One should note that the existence of other terms are not seen from the boundary theory to this level of approximation. Their behaviour near the boundary however, is pointing what kind of information from the boundary theory is missing to be able to reconstruct the bulk. Obviously more work is needed to refine and elucidate their meaning and interrelations in holographic setup.

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Cited by 1 Pith paper

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  1. Path Integral Approach to Quantum Fisher Information

    quant-ph 2026-04 unverdicted novelty 7.0

    The quantum Fisher information is reformulated as the connected symmetrized covariance of a time-integrated action deformation or as an insertion of the action derivative in the propagator within a path integral framework.