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A quick review on Loop Qunatum Cosmology. Yi Ling Center for Gravity and Relativistic Astrophysics Nanchang University, China Nov. 5, 2007. KITPC & CCAST Workshop, Beijing. Outlines. The framework of loop quantum cosmology 1. The classical framework
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A quick review on Loop Qunatum Cosmology Yi Ling Center for Gravity and Relativistic Astrophysics Nanchang University, China Nov. 5, 2007 KITPC & CCAST Workshop, Beijing
Outlines • The framework of loop quantum cosmology 1. The classical framework 2. Quantum theory • The resolution of cosmological singularity • Effective formalism and inflation
gr-qc/0702030, Ashtekar • gr-qc/0304074, Ashtekar, Bojowald, Lewandowski • gr-qc/0601085, Bojowald
The WDW theory • Good semi-classical limit. • No improvement on the classical short distance disasters like cosmological singularity. • The key differences from WDW theory in LQC • The classical framework is constructed based on the holonomy of SU(2) connection . • In quantum theory, Bohr compactification of the configuration space is employed in order to construct the representation of the holonomy algebras • The differential equation is replaced by the difference equation.
x The WDW theory LQC
The Classical framework • A quick view on standard FRW cosmology
The Classical framework Conjugate momenta Where In general constraints become
The Classical framework Ashtekar-Sen variables: SU(2) connection Barbero-Immirzi parameter A triplet vector field with density weight one
The Classical framework In the present isotropic and homogeneous setting Fiducial metric: Physical metric:
The Classical framework The Hamiltonian constraint in full theory: In cosmological setting, it reduces to Thus, the total Hamiltonian constraint reads as Where
The Quantum theory • The phase space of gravity part • The Hilbert space The almost periodic functions constitute an ortho-normal basis in
The Quantum theory • Almost periodic functions
The Quantum theory • The action of the conjugate momentum Another well-defined operator: • The eigenbras and eigenvalues of volume operator:
The Quantum theory • The operator is well defined unitary operator, • but fails to be continuous with respect to • There is no operator corresponding to c on the Hilbert space • The well defined fundamental operators Related to the holonomy of connection.
The Quantum theory • The holonomy along the segment of length • in the i-th direction
The Quantum theory Classical constraints in full theory : (a) (b) After regularization
The Quantum theory The constraint in terms of well-defined fundamental variables:
The resolution of cosmological singularity The physical state Big bang corresponds to the state Given initial states One may determine all
The resolution of cosmological singularity • Cosmological singularity Closed universe:k=1, Scale factor Originated from a big-bang
The resolution of cosmological singularity Only valid at classical level
Effective formalism and inflation The effective or “semi-classical” Friedmann equations from LQC receive corrections from the following two facts : 1. The replacement of the inverse of scale factor: 2. The holonomy corrections.
Effective formalism and inflation The operator corresponding to the inverse of scale factor In standard quantum mechianics:
Effective formalism and inflation Ambiguities at semi-classical limit: 1. The representations of SU(2) for holonomy. 2. The operator ordering. j l
Effective formalism and inflation In general case
Effective formalism and inflation Effective Friedmann euqations:
Effective formalism and inflation 2. The holonomy corrections
Effective formalism and inflation From these effective equations, the following relevant phenomena have been investigated: 1. Super-inflation and inflations due to quantum geometry. 2. The big bounce universe. 3. The cosmological perturbation theory and scale invariance . 4. The resolution of the big rip in phantom cosmology.