Dual linearized gravity in D=6 coupled to a purely spin-two field of mixed symmetry (2,2)

Physics – High Energy Physics – High Energy Physics - Theory

Scientific paper

Rate now

  [ 0.00 ] – not rated yet Voters 0   Comments 0

Details

35 pages

Scientific paper

10.1002/prop.200900092

Under the hypotheses of analyticity, locality, Lorentz covariance, and Poincare invariance of the deformations, combined with the requirement that the interaction vertices contain at most two spatiotemporal derivatives of the fields, we investigate the consistent interactions between a single massless tensor field with the mixed symmetry (3,1) and one massless tensor field with the mixed symmetry (2,2). The computations are done with the help of the deformation theory based on a cohomological approach, in the context of the antifield-BRST formalism. Our result is that dual linearized gravity in D=6 gets coupled to a purely spin-two field with the mixed symmetry of the Riemann tensor such that both the gauge transformations and first-order reducibility relations in the (3,1) sector are changed, but not the gauge algebra.

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

Dual linearized gravity in D=6 coupled to a purely spin-two field of mixed symmetry (2,2) 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 Dual linearized gravity in D=6 coupled to a purely spin-two field of mixed symmetry (2,2), we encourage you to share that experience with our LandOfFree.com community. Your opinion is very important and Dual linearized gravity in D=6 coupled to a purely spin-two field of mixed symmetry (2,2) will most certainly appreciate the feedback.

Rate now

     

Profile ID: LFWR-SCP-O-588753

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