Chern-Simons term at finite density

Details Chern-Simons term at finite density Chern-Simons term at finite density

1996-12-12

arxiv.org/abs/hep-th/9612140v2

Phys.Lett. B403 (1997) 75-79

Physics

High Energy Physics

High Energy Physics - Theory

5 pages

Scientific paper

10.1016/S0370-2693(97)00493-0

The Chern-Simons topological term coefficient is derived at arbitrary finite density. As it occures that $\mu^2 = m^2$ is the crucial point for Chern-Simons. So when $\mu^2 < m^2 \mu$--influence disappears and we get the usual Chern-Simons term. On the other hand when $\mu^2 > m^2$ the Chern-Simons term vanishes because of non-zero density of background fermions. In particular for massless case parity anomaly is absent at any finite density. This result holds in any odd dimension as in abelian so as in nonabelian cases.

Affiliated with

Also associated with

No associations

Rating

Chern-Simons term at finite density 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 Chern-Simons term at finite density, we encourage you to share that experience with our LandOfFree.com community. Your opinion is very important and Chern-Simons term at finite density will most certainly appreciate the feedback.

Rate now

Comments { 0 }

Profile ID: LFWR-SCP-O-623639