Fricke S-duality in CHL models
Daniel Persson (Fundamental Physics, Chalmers University of Technology, 41296, Gothenburg, Sweden); Roberto Volpato (Theory Group, SLAC National Accelerator Laboratory, 2575 Sand Hill Road, Menlo Park, CA, 94025, U.S.A., Stanford Institute for Theoretical Physics, Department of Physics, Stanford University, 382 Via Pueblo Mall, Stanford, CA, 94305, U.S.A.)
We consider four dimensional CHL models with sixteen spacetime supersymmetries obtained from orbifolds of type IIA superstring on K3× T 2 by a ℤ N $$ {\mathrm{\mathbb{Z}}}_N $$ symmetry acting (possibly) non-geometrically on K3. We show that most of these models (in particular, for geometric symmetries) are self-dual under a weak-strong duality acting on the heterotic axio-dilaton modulus S by a “Fricke involution” S → −1 /NS . This is a novel symmetry of CHL models that lies outside of the standard S L 2 ℤ $$ \mathrm{S}\mathrm{L}\left(2,\mathrm{\mathbb{Z}}\right) $$ -symmetry of the parent theory, heterotic strings on T 6 . For self-dual models this implies that the lattice of purely electric charges is N -modular, i.e. isometric to its dual up to a rescaling of its quadratic form by N . We verify this prediction by determining the lattices of electric and magnetic charges in all relevant examples. We also calculate certain BPS-saturated couplings and verify that they are invariant under the Fricke S-duality. For CHL models that are not self-dual, the strong coupling limit is dual to type IIA compactified on T 6 / ℤ N $$ {T}^6/{\mathrm{\mathbb{Z}}}_N $$ , for some ℤ N $$ {\mathrm{\mathbb{Z}}}_N $$ -symmetry preserving half of the spacetime supersymmetries.
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