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Brane world effective actions for D-branes with fluxes

Matteo Bertolini, Marco Billo, Alberto Lerda, Jose F. Morales, Rodolfo Russo

Abstract

We develop systematic string techniques to study brane world effective actions for models with magnetized (or equivalently intersecting) D-branes. In particular, we derive the dependence on all NS-NS moduli of the kinetic terms of the chiral matter in a generic non-supersymmetric brane configurations with non-commuting open string fluxes. Near a N=1 supersymmetric point the effective action is consistent with a Fayet-Iliopoulos supersymmetry breaking and the normalization of the scalar kinetic terms is nothing else than the Kahler metric. We also discuss, from a stringy perspective, D and F term breaking mechanisms, and how, in this generic set up, the Kahler metric enters in the physical Yukawa couplings.

Brane world effective actions for D-branes with fluxes

Abstract

We develop systematic string techniques to study brane world effective actions for models with magnetized (or equivalently intersecting) D-branes. In particular, we derive the dependence on all NS-NS moduli of the kinetic terms of the chiral matter in a generic non-supersymmetric brane configurations with non-commuting open string fluxes. Near a N=1 supersymmetric point the effective action is consistent with a Fayet-Iliopoulos supersymmetry breaking and the normalization of the scalar kinetic terms is nothing else than the Kahler metric. We also discuss, from a stringy perspective, D and F term breaking mechanisms, and how, in this generic set up, the Kahler metric enters in the physical Yukawa couplings.

Paper Structure

This paper contains 20 sections, 169 equations, 3 figures.

Figures (3)

  • Figure 1: The tetrahedron in $\theta$-space.
  • Figure 2: a) Classical contributions $\mathcal{W}_{IJK}$ to the Yukawa couplings in intersecting D-brane models. b) Quantum contributions $\mathcal{A}_{IJK}$ are given by string correlators
  • Figure 3: The reflection matrices $R_0$ and $R_\pi$ and the monodromy matrices $R = R_\pi^{-1} R_0$ for the three twisted open strings. The matrices pertaining to the different strings are labeled by the angles $\theta$, $\nu$, $\omega$ which determine the eigenvalues of the monodromy according to Eq. (\ref{['diagonalR1']}).