2011
DOI: 10.1002/prop.201100087
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Kähler metrics and gauge kinetic functions for intersecting D6‐branes on toroidal orbifolds – The complete perturbative story

Abstract: We systematically derive the perturbatively exact holomorphic gauge kinetic function, the open string Kähler metrics and closed string Kähler potential on intersecting D6-branes by matching open string one-loop computations of gauge thresholds with field theoretical gauge couplings in N = 1 supergravity. We consider all cases of bulk, fractional and rigid D6-branes on T 6 /ΩR and the orbifolds T 6 /(Z N × ΩR) and T 6 /(Z 2 × Z 2M × ΩR) without and with discrete torsion, which differ in the number of bulk compl… Show more

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Cited by 31 publications
(76 citation statements)
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References 81 publications
(390 reference statements)
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“…Massless open string excitations arise at the intersection points of two distinct D6-branes wrapping supersymmetric three-cycles and fill out supermultiplets of the supersymmetry algebra generated by the mutually unbroken supercharges. Furthermore, on toroidal orbifold backgrounds the Kähler metrics for these open string states can be computed as a function of the closed string moduli [87][88][89][90]. The type of matter (and subsequently the functional dependence of the Kähler metrics) depends on the codimension of the intersection Π α ∩ Π β = 0 in the ambient space T 6 : The Kähler metric for an open string modulus Φ i along two-torus T 2 (i) can be written (at leading order) as a rational function of the closed string moduli:…”
Section: Toroidal Orbifolds and Kähler Metricsmentioning
confidence: 99%
“…Massless open string excitations arise at the intersection points of two distinct D6-branes wrapping supersymmetric three-cycles and fill out supermultiplets of the supersymmetry algebra generated by the mutually unbroken supercharges. Furthermore, on toroidal orbifold backgrounds the Kähler metrics for these open string states can be computed as a function of the closed string moduli [87][88][89][90]. The type of matter (and subsequently the functional dependence of the Kähler metrics) depends on the codimension of the intersection Π α ∩ Π β = 0 in the ambient space T 6 : The Kähler metric for an open string modulus Φ i along two-torus T 2 (i) can be written (at leading order) as a rational function of the closed string moduli:…”
Section: Toroidal Orbifolds and Kähler Metricsmentioning
confidence: 99%
“…Predictions for kinetic mixing and its phenomenology were considered in type II strings in [20][21][22][23][24][25][26][27][28][29]; in [24,28] both masses and mixings were studied, and it was argued that the Dark Force scenario could be accommodated provided that there is additional sequestering. However, it is to heterotic orbifolds that we shall turn in this paper.…”
Section: Jhep01(2012)021mentioning
confidence: 99%
“…We aim at extending the search for global three‐generation PS models by the analysis of different choices of the involution R, and we will classify the type of symmetry enhancement [USporSO] based on conformal field theory methods, see e.g. . Last but not least, studying non‐factorisable tori is motivated by moduli stabilisation involving closed string background fluxes, which we plan to address in the future.…”
Section: Results and Outlookmentioning
confidence: 99%