Generalized conformal quantum mechanics as an ideal observer in two-dimensional gravity

Fuente: arXiv
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Main Authors: Banerjee, Archi, Kibe, Tanay, Molina, Martín, Mukhopadhyay, Ayan
Format: Preprint
Published: 2024
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author Banerjee, Archi
Kibe, Tanay
Molina, Martín
Mukhopadhyay, Ayan
author_facet Banerjee, Archi
Kibe, Tanay
Molina, Martín
Mukhopadhyay, Ayan
contents We obtain an action for a generalized conformal mechanics (GCM) coupled to Jackiw-Teitelboim (JT) gravity from a double scaling limit of the motion of a charged massive particle in the near-horizon geometry of a near-extremal spherical black hole. When JT gravity is treated in the classical approximation, the backreaction of the particle's wavefunction on the time-reparametrization mode (and therefore the bulk metric) vanishes while the conformal symmetry in GCM is reparametrized in a state-dependent way. We also construct the semi-classical Hilbert space of the full theory by explicitly solving the general time-dependent normalizable solutions of the Schrödinger equation for GCM, and show that the time-reparametrization mode can be inferred from the measurement of suitable observables. Since the full theory of the GCM coupled to JT gravity is amenable to quantization, it can lead to a solvable model for a detector coupled to quantum gravity.
format Preprint
id arxiv_https___arxiv_org_abs_2409_15415
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle Generalized conformal quantum mechanics as an ideal observer in two-dimensional gravity
Banerjee, Archi
Kibe, Tanay
Molina, Martín
Mukhopadhyay, Ayan
High Energy Physics - Theory
General Relativity and Quantum Cosmology
Quantum Physics
We obtain an action for a generalized conformal mechanics (GCM) coupled to Jackiw-Teitelboim (JT) gravity from a double scaling limit of the motion of a charged massive particle in the near-horizon geometry of a near-extremal spherical black hole. When JT gravity is treated in the classical approximation, the backreaction of the particle's wavefunction on the time-reparametrization mode (and therefore the bulk metric) vanishes while the conformal symmetry in GCM is reparametrized in a state-dependent way. We also construct the semi-classical Hilbert space of the full theory by explicitly solving the general time-dependent normalizable solutions of the Schrödinger equation for GCM, and show that the time-reparametrization mode can be inferred from the measurement of suitable observables. Since the full theory of the GCM coupled to JT gravity is amenable to quantization, it can lead to a solvable model for a detector coupled to quantum gravity.
title Generalized conformal quantum mechanics as an ideal observer in two-dimensional gravity
topic High Energy Physics - Theory
General Relativity and Quantum Cosmology
Quantum Physics
url https://arxiv.org/abs/2409.15415