Gauge procedure with gauge fields of various ranks

Physics – High Energy Physics – High Energy Physics - Theory

Scientific paper

Rate now

  [ 0.00 ] – not rated yet Voters 0   Comments 0

Details

References added

Scientific paper

10.1016/j.physleta.2004.08.002

The standard procedure for making a global phase symmetry local involves the introduction of a rank 1, vector field in the definition of the covariant derivative. Here it is shown that it is possible to gauge a phase symmetry using fields of various ranks. In contrast to other formulations of higher rank gauge fields we begin with the coupling of the gauge field to some matter field, and then derive the gauge invariant, field strength tensor. Some of these gauge theories are similar to general relativity in that their covariant derivatives involve derivatives of the rank n gauge field rather than just the gauge field. For general relativity the covariant derivative involves the Christoffel symbols which are written in terms of derivatives of the metric tensor. Many (but not all) of the Lagrangians that we find for these higher rank gauge theories lead to nonrenormalizable quantum theories which is also similar to general relativity.

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

Gauge procedure with gauge fields of various ranks 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 Gauge procedure with gauge fields of various ranks, we encourage you to share that experience with our LandOfFree.com community. Your opinion is very important and Gauge procedure with gauge fields of various ranks will most certainly appreciate the feedback.

Rate now

     

Profile ID: LFWR-SCP-O-584870

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