$(p+2)$-form gauge fields for $p$-brane through an action-at-a-distance

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dc.creatorMiyazaki, T.
dc.creatorOhzeki, C.
dc.creatorYamanobe, M.
dc.date1997-12-26
dc.date.accessioned2026-07-07T04:24:03Z
dc.date.available2026-07-07T04:24:03Z
dc.descriptionIn 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 $ϕ^{(p+1)}\to ϕ^{(p+1)}+dΛ^{(p)}$ 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: $ϕ^{(p+2)}\to ϕ^{(p+2)} +δΛ^{(p+3)}$, with $δ$, a coboundary operator.
dc.description6 pages
dc.identifierhttps://arxiv.org/abs/hep-th/9712234
dc.identifierhttp://arxiv.org/abs/hep-th/9712234
dc.identifierNuovo Cim. B114 (1999) 589-593
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/55265
dc.subjectHigh Energy Physics - Theory
dc.title$(p+2)$-form gauge fields for $p$-brane through an action-at-a-distance
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