Physical states in $N = 1$ supergravity

Details Physical states in $N = 1$ supergravity Physical states in $N = 1$ supergravity

1993-04-20

arxiv.org/abs/hep-th/9304084v1

Phys.Lett. B321 (1994) 368-371

Physics

High Energy Physics

High Energy Physics - Theory

9 pages, DAMTP Preprint DAMTP-R-93-4

Scientific paper

10.1016/0370-2693(94)90259-3

By solving the supersymmetry constraints for physical wave-functions, it is shown that the only two allowed bosonic states in $ N = 1 $ supergravity are of the form const.~exp~$(\pm I / \hbar) $, where $ I $ is an action functional of the three-metric. States containing a finite number of fermions are forbidden. In the case that the spatial topology is $ S^3 $, the state const.~exp~$(- I / \hbar)$ is the wormhole ground state, and the state const.~exp~$(I / \hbar)$ is the Hartle--Hawking state. $ N = 1 $ supergravity has no quantum ultraviolet divergences, and no quantum corrections.

Affiliated with

Also associated with

No associations

Rating

Physical states in $N = 1$ supergravity does not yet have a rating. At this time, there are no reviews or comments for this scientific paper.

If you have personal experience with Physical states in $N = 1$ supergravity, we encourage you to share that experience with our LandOfFree.com community. Your opinion is very important and Physical states in $N = 1$ supergravity will most certainly appreciate the feedback.

Rate now

Comments { 0 }

Profile ID: LFWR-SCP-O-394750