D-branes, supersymmetry breaking, and neutrinos

This thesis studies meta- and exactly stable supersymmetry breaking mechanisms in heterotic and type IIB string theories and constructs an F-theory Grand Unified Theory model for neutrino physics in which neutrino mass is determined by the supersymmetry breaking mechanism.;Focussing attention on heterotic string theory compactified on a 4-torus, stability of non-supersymmetric states is studied. A non-supersymmetric state with robust stability is constructed, and its exact stability is proven in a large region of moduli space of T4 against all the possible decay mechanisms allowed by charge conservation. Using string-string duality, the results are interpreted in terms of Dirichlet-branes in type IIA string theory compactified on an orbifold limit of a K3 surface.;In type IIB string theory, metastable and exactly stable non-supersymmetric systems are constructed using D-branes and Calabi-Yau geometry. Branes and anti-branes wrap rigid and separate 2-spheres inside a non-compact Calabi-Yau three-fold: supersymmetry is spontaneously broken. These metastable vacua are analyzed in a holographic dual picture on a complex-deformed Calabi-Yau three-fold where 2-spheres have been replaced by 3-spheres with flux through them. By computing bosonic masses, we identify location and mode of instability. The moduli space of this complex-deformed Calabi-Yau three-fold is studied, and methods for studying the global phase structure of supersymmetric and non-supersymmetric flux vacua are proposed. By turning on a varying Neveu-Schwarz flux inside the Calabi-Yau three-fold, we build meta- and exactly stable non-supersymmetric configurations with D-branes but with no anti-D-branes.;Finally, a scenario for Dirac neutrinos in an F-theory SU(5) GUT model is proposed. Supersymmetry breaking leads to an F-term for Higgs field H†d of order FHd ∼ muHu ∼ M2weak which induces a Dirac mass of mnu ∼ M2weak /ΛUV. A mild normal hierarchy with masses ( m3, m2, m 1) ∼ 50 x (1, a1/2GUT,a GUT ) meV and large mixing angles theta23 ∼ theta 12 > theta13 ∼ thetaC ∼ a1/2GUT ∼ 0.2 are predicted.