Einstein-Cartan geometry in CDT?

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In summary, Einstein-Cartan geometry is a type of geometric framework that extends Einstein's theory of general relativity to include the intrinsic spin of particles. It is applied in CDT to describe the discrete spacetime structure of the theory and allows for the incorporation of both curvature and spin. The main differences between Einstein-Cartan geometry and general relativity are the inclusion of spin and the possibility of torsion. Its use in CDT could potentially lead to a better understanding of matter and energy at a quantum level and has implications for our understanding of the fundamental nature of the universe. It also contributes to the search for a theory of quantum gravity by offering a unique perspective and allowing for the exploration of discrete spacetime structures.
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Orbb
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I hope I do not ask a dumb question: Does/did ever the causal dynamical triangulation program implement torsion degrees of freedom when calculating exp(iS)? Or were the calculations performed torsion-free? I did a search but couldn't figure it out.
 
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In EC theory, torsion is non-propagating, so there are no torsion waves. Therefore torsions exists only in the world-volume where its source, namely the matter spin current is non-vanishing.

As far as I know CDT has not yet included matter degrees of freedom, therefore torsion is always zero.
 
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I see. Thank you!
 

Related to Einstein-Cartan geometry in CDT?

1. What is Einstein-Cartan geometry?

Einstein-Cartan geometry is a type of geometric framework that extends Einstein's theory of general relativity to include the intrinsic spin of particles, as described by Cartan's theory of spinors. It allows for a more comprehensive understanding of the curvature of spacetime and the behavior of matter and energy within it.

2. How is Einstein-Cartan geometry applied in CDT?

CDT, or Causal Dynamical Triangulations, is a quantum gravity theory that combines the principles of general relativity with those of quantum mechanics. Einstein-Cartan geometry is used in CDT to describe the discrete spacetime structure, or "building blocks," on which the theory is based. It allows for the incorporation of both curvature and spin into the model.

3. What are the main differences between Einstein-Cartan geometry and general relativity?

The main difference is the incorporation of intrinsic spin into the theory. In general relativity, gravity is described solely by the curvature of spacetime, while in Einstein-Cartan geometry, the spin of particles also plays a role in the behavior of gravity. Additionally, Einstein-Cartan geometry allows for torsion, or the twisting of spacetime, which is not included in general relativity.

4. What are some potential implications of using Einstein-Cartan geometry in CDT?

One potential implication is the ability to better understand the behavior of matter and energy at a quantum level in the presence of gravity. Einstein-Cartan geometry also allows for the possibility of describing spacetime as discrete building blocks, rather than a continuous fabric, which could have implications for our understanding of the fundamental nature of the universe.

5. How does Einstein-Cartan geometry in CDT contribute to the search for a theory of quantum gravity?

Einstein-Cartan geometry in CDT is one of many approaches being explored in the search for a theory of quantum gravity. It offers a unique perspective by incorporating both curvature and spin into the model, which could potentially lead to a more comprehensive understanding of the behavior of matter and energy at a quantum level in the presence of gravity. Its use in CDT also allows for the exploration of discrete spacetime structures, which could have implications for the unification of quantum mechanics and general relativity.

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