Abstract

Quantum gravity is expected to be necessary in order to understand situations where classical general relativity breaks down. In particular in cosmology one has to deal with initial singularities, i.e., the fact that the backward evolution of a classical space-time inevitably comes to an end after a finite amount of proper time. This presents a breakdown of the classical picture and requires an extended theory for a meaningful description. Since small length scales and high curvatures are involved, quantum effects must play a role. Not only the singularity itself but also the surrounding space-time is then modified. One particular realization is loop quantum cosmology, an application of loop quantum gravity to homogeneous systems, which removes classical singularities. Its implications can be studied at different levels. Main effects are introduced into effective classical equations which allow to avoid interpretational problems of quantum theory. They give rise to new kinds of early universe phenomenology with applications to inflation and cyclic models. To resolve classical singularities and to understand the structure of geometry around them, the quantum description is necessary. Classical evolution is then replaced by a difference equation for a wave function which allows to extend space-time beyond classical singularities. One main question is how these homogeneous scenarios are related to full loop quantum gravity, which can be dealt with at the level of distributional symmetric states. Finally, the new structure of space-time arising in loop quantum gravity and its application to cosmology sheds new light on more general issues such as time.Electronic Supplementary MaterialSupplementary material is available for this article at 10.12942/lrr-2005-11.

Highlights

  • The date given as uniquely identifies the version of the article you are referring to

  • Loop quantum cosmology is based on quantum Riemannian geometry, or loop quantum gravity [172, 22, 195, 174], which is an attempt at a non-perturbative and background independent quantization of general relativity

  • Loop cosmology is an effective description of quantum effects in cosmology, obtained in a framework of a background independent and non-perturbative quantization

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Summary

Introduction

While general relativity is very successful in describing the gravitational interaction and the structure of space and time on large scales [205], quantum gravity is needed for the small-scale behavior. This is usually relevant when curvature, or in physical terms energy densities and tidal forces, becomes large. That the classical theory by itself cannot be sufficient to describe the history in a well-defined way is illustrated by singularity theorems [123] which apply in this case: After a finite time of backward evolution the classical universe will collapse into a single point and energy densities diverge. This review is intended to give an overview and summary of the current status of those problems, in particular in the new framework of loop quantum cosmology

The Viewpoint of Loop Quantum Cosmology
Loop Quantum Gravity
Geometry
Ashtekar variables
Representation
Function spaces
Composite operators
Hamiltonian constraint
Open issues
Loop Cosmology
Isotropy
Collapsing phase
Expansion
Model building
Stability
Anisotropies
Anisotropy
Isotropization
Bianchi IX
Isotropic curvature suppression
4.10 Anisotropy
4.11 Inhomogeneities
4.12 Inhomogeneous matter with isotropic quantum geometry
4.13 Inhomogeneity
4.14 Inhomogeneous models
Results
4.15.1 Matter gradient terms and small-a effects
4.15.2 Matter gradient terms and large-a effects
4.15.3 Non-inflationary structure formation
4.15.4 Stability
4.16 Summary
Loop quantization of symmetric models
Symmetries and backgrounds
Semiclassical limit and correction terms
WKB approximation
Effective formulation
Homogeneity
Diagonalization
Inhomogeneous models
5.10 Einstein–Rosen waves
5.10.1 Canonical variables
5.10.2 Representation
5.11 Spherical symmetry
5.12 Loop inspired quantum cosmology
5.13 Dynamics
5.14 Dynamics
5.15 Singularities
5.17 Pre-classicality and boundedness
5.18 Dynamical initial conditions
5.19 Summary
Models within the Full Theory
Symmetric states
Basic operators
Quantization before reduction
Minisuperspace approximation
Quantum geometry from models to the full theory
Philosophical Ramifications
The role of time
Determinism
Conceptual issues
Mathematical development of models
Applications
Homogeneous models
Outlook
Partial backgrounds
Classification of symmetric principal fiber bundles
Classification of invariant connections
Isotropic models
Spherical symmetry
Full Text
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