Jump to content

Dirac equation in curved spacetime

From Wikipedia, the free encyclopedia

This is an old revision of this page, as edited by 68.129.124.6 (talk) at 20:06, 8 January 2021. The present address (URL) is a permanent link to this revision, which may differ significantly from the current revision.

In mathematical physics, the Dirac equation in curved spacetime generalizes the original Dirac equation to curved space.

It can be written by using vierbein fields and the gravitational spin connection. The vierbein defines a local rest frame, allowing the constant Gamma matrices to act at each spacetime point. In this way, Dirac's equation takes the following form in curved spacetime:[1]

Here eaμ is the vierbein and Dμ is the covariant derivative for fermionic fields, defined as follows

where σab is the commutator of Gamma matrices:

and ωμab are the spin connection components.

Note that here Latin indices denote the "Lorentzian" vierbein labels while Greek indices denote manifold coordinate indices.

See also

References

  1. ^ Lawrie, Ian D. A Unified Grand Tour of Theoretical Physics.