Hodge decomposition theorem for Abelian two form gauge theory

Physics – High Energy Physics – High Energy Physics - Theory

Scientific paper

Rate now

  [ 0.00 ] – not rated yet Voters 0   Comments 0

Details

LaTeX, 18 pages, no figures, minor corrections, references updated, typos corrected, journal reference given

Scientific paper

10.1088/0305-4470/33/40/312

We show that the BRST/anti-BRST invariant 3+1 dimensional 2-form gauge theory has further nilpotent symmetries (dual BRST /anti-dual BRST) that leave the gauge fixing term invariant. The generator for the dual BRST symmetry is analogous to the co-exterior derivative of differential geometry. There exists a bosonic symmetry which keeps the ghost terms invariant and it turns out to be the analogue of the Laplacian operator. The Hodge duality operation is shown to correspond to a discrete symmetry in the theory. The generators of all these continuous symmetries are shown to obey the algebra of the de Rham cohomology operators of differential geometry. We derive the extended BRST algebra constituted by six conserved charges and discuss the Hodge decomposition theorem in the quantum Hilbert space of states.

No associations

LandOfFree

Say what you really think

Search LandOfFree.com for scientists and scientific papers. Rate them and share your experience with other people.

Rating

Hodge decomposition theorem for Abelian two form gauge theory 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 Hodge decomposition theorem for Abelian two form gauge theory, we encourage you to share that experience with our LandOfFree.com community. Your opinion is very important and Hodge decomposition theorem for Abelian two form gauge theory will most certainly appreciate the feedback.

Rate now

     

Profile ID: LFWR-SCP-O-144334

  Search
All data on this website is collected from public sources. Our data reflects the most accurate information available at the time of publication.