1997
DOI: 10.1016/s0550-3213(96)00514-7
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Aspects of type I-type II-heterotic triality in four dimensions

Abstract: We discuss the equivalence between Type I, Type II and Heterotic N = 2 superstring theories in four dimensions. We study the effective field theory of Type I models obtained by orientifold reductions of Type IIB compactifications on K 3 × T 2 . We show that the perturbative prepotential is determined by the one-loop corrections to the Planck mass and is associated to an index. As is the case for threshold corrections to gauge couplings, this renormalization is entirely due to N = 2 BPS states that originate fr… Show more

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Cited by 127 publications
(311 citation statements)
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“…We will proof that the normalization of the partition function is given by (23) in the case that N is prime. The proof in the general case N ∈ N relies on the fact that every natural number can uniquely be written as a product of prime numbers and is quite lengthy as there are sectors with hv i ∈ Z and one has more cases to consider.…”
Section: B2 General Nmentioning
confidence: 93%
“…We will proof that the normalization of the partition function is given by (23) in the case that N is prime. The proof in the general case N ∈ N relies on the fact that every natural number can uniquely be written as a product of prime numbers and is quite lengthy as there are sectors with hv i ∈ Z and one has more cases to consider.…”
Section: B2 General Nmentioning
confidence: 93%
“…In refs. [47,48], however, a simple, "lowest order", description in terms of another, extended, cubic prepotential was proposed: 10) where y r 3 (r = 1, . .…”
Section: Classical Effective Action With D3-branesmentioning
confidence: 99%
“…More precisely, if one follows [27,28,29] and describes the "lowest order" theory at the N = 2 level in terms of a cubic holomorphic prepotential F (t) = c ijk t i t j t k , where t i denote the moduli living in vector multiplets, the resulting Kähler potential, K, only depends on the imaginary parts of the moduli: K = K(t i −t i ). 5 Moreover, for the particular cubic prepotential suggested in [47,48], it was observed in [16] that the relevant D7-gauge couplings (still at the N = 2 level) likewise do not depend on the real part of y 3 . This inflaton shift symmetry is not expected to survive all quantum corrections (e.g.…”
Section: Introductionmentioning
confidence: 98%
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