Group theoretical Quantization of Isotropic Loop Cosmology

TL;DR

This paper develops a group theoretical quantization method for isotropic loop cosmology, using SU(1,1) symmetry to describe quantum dynamics and resolve the big bang singularity with coherent states.

Contribution

It introduces a novel SU(1,1) group approach to quantize loop cosmology, ensuring anomaly-free superselection sectors and clear semiclassical states.

Findings

Successful quantization with SU(1,1) symmetry

Explicit construction of coherent states

Clear description of the quantum bounce

Abstract

We achieve a group theoretical quantization of the flat Friedmann-Robertson-Walker model coupled to a massless scalar field adopting the improved dynamics of loop quantum cosmology. Deparemeterizing the system using the scalar field as internal time, we first identify a complete set of phase space observables whose Poisson algebra is isomorphic to the su(1,1) Lie algebra. It is generated by the volume observable and the Hamiltonian. These observables describe faithfully the regularized phase space underlying the loop quantization: they account for the polymerization of the variable conjugate to the volume and for the existence of a kinematical non-vanishing minimum volume. Since the Hamiltonian is an element in the su(1,1) Lie algebra, the dynamics is now implemented as SU(1,1) transformations. At the quantum level, the system is quantized as a time-like irreducible representation of the group SU(1,1). These representations are labeled by a half-integer spin, which gives the minimal volume. They provide superselection sectors without quantization anomalies and no factor ordering ambiguity arises when representing the Hamiltonian. We then explicitly construct SU(1,1) coherent states to study the quantum evolution. They not only provide semiclassical states but truly dynamical coherent states. Their use further clarifies the nature of the bounce that resolves the big bang singularity.