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On RR couplings on D-branes at order O(α2)O(\alpha'^2)

Abstract

Recently, it has been found that there are couplings of the RR field strength F(p)F^{(p)} and the B-field strength HH on the world volume of Dp_p-branes at order O(α2){\cal O}(\alpha'^2). These couplings which have both world-volume and transverse indices, are invariant under the linear T-duality transformations. Consistency with the nonlinear T-duality indicates that the RR field strength F(p)F^{(p)} in these couplings should be replaced by F(p)=dC(p1){\cal F}^{(p)}=d{\cal C}^{(p-1)} where C=eBC{\cal C}=e^{B}C. This replacement, however, reproduces some non-gauge invariant terms. On the other hand, the nonlinear terms are invariant under the linear T-duality transformations at the level of two B-fields. This allows one to remove some of the nonlinear terms in F(p){\cal F}^{(p)}. We fix this by comparing the nonlinear couplings with the S-matrix element of one RR and two NSNS vertex operators. Our results indicate that in the expansion of F(p){\cal F}^{(p)} one should keep only the B-field gauge invariant terms, e.g. BdC(p3)B\wedge dC^{(p-3)} where both indices of B-field lie along the brane. Moreover, in this case one should replace BB with B+2παfB+2\pi\alpha'f to have the BB-field gauge invariance.Comment: 23 pages, Latex file, 1 figure; v2:typos corrected, to appear in JHE

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