- #1
IRobot
- 87
- 0
Hi, I have two questions dealing with general relativity:
-assume that we want to use a manifold with torsion, an we also want to add electromagnetism, Faraday's tensor ([tex]F^{\mu\nu}=\nabla^{\mu}A^{\nu}-\nabla^{\nu}A^{\mu}[/tex]) is no longer gauge-invariant, I have been looking for a way of constructing a cinetic term for the vector field which is gauge invariant without any results, maybe electromagnetism forbids the manifold from having torsion
-in the prologue of Kiritsis book on String Theory, he writes: "Three of the four fundamental forces known are described by gauge theories. The fourth, gravity, is also based on local gauge invariance, albeit of a different type, and so far stands apart." I know that this gauge transformation is [tex] g^{\alpha\beta} \rightarrow g^{\alpha\beta} + \partial^{\alpha}\epsilon^{\beta} + \partial^{\beta}\epsilon^{\alpha} [/tex] the infinitesimal form of a diffeomorphism transformation, but I don't see the conceptual difference with local U(1), SU(2), or SU(3) gauge transformation.Thanks.
-assume that we want to use a manifold with torsion, an we also want to add electromagnetism, Faraday's tensor ([tex]F^{\mu\nu}=\nabla^{\mu}A^{\nu}-\nabla^{\nu}A^{\mu}[/tex]) is no longer gauge-invariant, I have been looking for a way of constructing a cinetic term for the vector field which is gauge invariant without any results, maybe electromagnetism forbids the manifold from having torsion
-in the prologue of Kiritsis book on String Theory, he writes: "Three of the four fundamental forces known are described by gauge theories. The fourth, gravity, is also based on local gauge invariance, albeit of a different type, and so far stands apart." I know that this gauge transformation is [tex] g^{\alpha\beta} \rightarrow g^{\alpha\beta} + \partial^{\alpha}\epsilon^{\beta} + \partial^{\beta}\epsilon^{\alpha} [/tex] the infinitesimal form of a diffeomorphism transformation, but I don't see the conceptual difference with local U(1), SU(2), or SU(3) gauge transformation.Thanks.