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Spontaneous splitting and internal isometries of superstring vacua
Journal of Mathematical Physics, 1987Superstring vacua are normally presumed to be of the form M×K, where dim(M)=4, dim(K)=6, and where × denotes the global Riemannian product. Since, however, one would ultimately wish to understand the external/internal distinction in terms of some dynamical mechanism (‘‘spontaneous splitting’’) involving vacuum expectation values of local fields, it may
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(2, 2) VACUA OF THE HETEROTIC SUPERSTRING COMPACTIFIED ON SU(2)3 GROUPFOLDS
International Journal of Modern Physics A, 1991In this paper we classify the (2, 2) superstring vacua corresponding to non-linear σ-models on SU (2)3 groupfolds fermionized by 18 + 18 Majorana fermions. For the subclass of the completely bosonizable vacua, the generation number ½X is a multiple of 12 and the number of tangent-bundle deformations End(T) is a multiple of 4.
CASTELLANI, Leonardo +3 more
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Non-Compact Current Algebras and Heterotic Superstring Vacua
1990It has been shown that a four dimensional finite and consistent superstring theory [1] can be constructed by combining any 2-dimensional superconformai field theory with a central charge c=9 with a superstring propagating in flat 4-dimensional Minkowski space-time.
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Nonrenormalization of the superstring tension
Physical Review Letters, 1989Atish Dabholkar, Jeffrey A Harvey
exaly
Consistent Supergravity Theories and Superstring Vacua in Diverse Dimensions
2015Stoyanov, Boris, Heplab, Brane
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The N > 2 $$ \mathcal{N}>2 $$ supersymmetric AdS vacua in maximal supergravity
Journal of High Energy Physics, 2014Antonio Gallerati +2 more
exaly
Properties of superstring vacua from (topological) Landau-Ginzburg models
1998openaire +1 more source

