1988
DOI: 10.1016/0550-3213(88)90245-3
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Orbifold models and modular transformation

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Cited by 27 publications
(22 citation statements)
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“…Once the twist vector is set, different Z N orbifold models arise from the different gauge embeddings that satisfy the modular invariance conditions [51][52][53][54] which ensure an effective theory free of any anomalies. We are then interested in admissible shift vectors V and Wilson lines A i that comply with (no summation implied)…”
Section: Jhep01(2012)021mentioning
confidence: 99%
“…Once the twist vector is set, different Z N orbifold models arise from the different gauge embeddings that satisfy the modular invariance conditions [51][52][53][54] which ensure an effective theory free of any anomalies. We are then interested in admissible shift vectors V and Wilson lines A i that comply with (no summation implied)…”
Section: Jhep01(2012)021mentioning
confidence: 99%
“…Direct consequences of this are that not all the Wilson lines are non-trivial nor independent, they can take only quantised values, and their order N α is restricted by the geometry of the compact space. Demanding modular invariance of the one-loop vacuum-to-vacuum amplitudes imposes additional constraints on the orbifold parameters which, for N orbifolds without Wilson lines, read [38][39][40] N…”
Section: Jhep01(2011)071mentioning
confidence: 99%
“…For instance, if ϵ g corresponds to the generalized Gliozzi-Scherk-Olive (GSO) phase in heterotic orbifold models. By the GSO projection, we can obtain the twist invariant states [16,17], and also the total number of massless modes, by inserting it into the partition function [18,19].…”
Section: ð2:11þmentioning
confidence: 99%