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<record version="1" id="353">
 <title>Quantum Geometry</title>
 <name>QuantumGeometry</name>
 <created>2009-01-07 08:40:14</created>
 <modified>2009-01-07 08:40:14</modified>
 <type>Topic</type>
 <creator id="441" name="bci1"/>
 <modifier id="441" name="bci1"/>
 <author id="441" name="bci1"/>
 <classification>
	<category scheme="msc" code="03."/>
	<category scheme="msc" code="03.65.Fd"/>
 </classification>
 <synonyms>
	<synonym concept="Quantum Geometry" alias="Quantum Algebraic Topology"/>
 </synonyms>
 <keywords>
	<term>quantum operator algebras</term>
	<term>quantum geometry</term>
 </keywords>
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 <content>This is a contributed topic on:
\section{Quantum Geometry}
In 4 dimensions, one of the attractive programs of spacetime quantization is “quantum geometry”, often represented as “loop quantum gravity” .
Loop quantum gravity starts with a Hamiltonian formulation of the first order formalism, with constraints, written in analogy to the (3+1)-dimensional case   that take the form:

$$D_i E^{ia} =0$$,  $$ E^i_a R^a_{ij} =0,$$ and  
$$\epsilon_{abc}E^{ib}E^{jc}R^a_{ij}=0,$$

 
where the indices $i,j$ and $k$ are the spatial indices on a surface of constant time, $$E^{ia}= \epsilon^{ij}e^a_j$$, $D_i$  is the $SO(2,1)$  gauge-covariant derivative for the connection $\omega$, and the $R^a_{ij}$ are the spatial components of the curvature two-form.</content>
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