1997/12/26 by T. Miyazaki, C. Ohzeki, M. Yamanobe
Physics and Astronomy · #hep-th
published as Nuovo Cim. B114 (1999) 589-593 · 6 pages
arxiv created 1997/12/26 · arxiv updated 2009/11/30
In the conventional p-brane theory, a gauge (p+1)-form field ϕ(p+1) mediates the interaction between p-branes, which is gauge invariant in the sense ϕ(p+1)→ ϕ(p+1)+dΛ(p) with Λ(p), an arbitrary p-form and d, a boundary operator. We, on the contrary, propose to introduce a new gauge field ϕ(p+2) mediating the interaction, and we have a new type of gauge transformation: ϕ(p+2)→ ϕ(p+2) +δΛ(p+3), with δ, a coboundary operator.