Coherent states of quantum spacetimes for black holes and de Sitter spacetime

Abstract

We provide a group theory approach to coherent states describing quantum space-time and its properties. This provides a relativistic framework for the metric of a Riemmanian space with bosonic and fermionic coordinates, its continuum and discrete states, and a kind of {\it"quantum optics"} for the space-time. {\bf New} results of this paper are: (i) The space-time is described as a physical coherent state of the complete covering of the SL(2C) group, eg the Metaplectic group Mp(n). (ii) (The discrete structure arises from its two irreducible: $\text{even}$ $(2n)$ and $\text{odd}$ $(2n+1)$ representations, ($n=1,2,3...$ ), spanning the complete Hilbert space $\mathcal{H}={\mathcal{H}}_{odd}\oplus {\mathcal{H}}_{even}$. Such a global or {\it complete} covering guarantees the CPT symmetry and unitarity. Large $n$ yields the classical and continuum manifold, as it must be. (iii) The coherent and squeezed states and Wigner functions of quantum-space-time for black holes and de Sitter, and (iv) for the quantum space-imaginary time (instantons), black holes in particular. They encompass the semiclassical space-time behaviour plus high quantum phase oscillations, and notably account for the classical-quantum gravity duality and trans-Planckian domain. The Planck scale consistently corresponds to the coherent state eigenvalue $\alpha =0$ (and to the $n=0$ level in the discrete representation). It is remarkable the power of coherent states in describing both continuum and discrete space-time. The quantum space-time description is {\it regular}, there is no any space-time singularity here, as it must be.

47 pages, 4 Figures, Published in Physical Review D, 7 December 2023

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• Quantum Space-Time Symmetries: A Principle of Minimum Group Representation
• Entanglement and Generalized Berry Geometrical Phases in Quantum Gravity
• Classical (ontological) dual states in quantum theory and the minimal group representation Hilbert space