Sigma models with non-commuting complex structures and extended supersymmetry

We discuss additional supersymmetries for N = (2, 2) supersymmetric non-linear sigma models described by left and right semichiral superfields.Comment: 11 pages. Talk presented by U.L. at "30th Winter School on Geometry and Physics" Srni, Czech Republic January 2010

Hamiltonian construction of W-gravity actions

We show that all W-gravity actions can be easilly constructed and understood from the point of view of the Hamiltonian formalism for the constrained systems. This formalism also gives a method of constructing gauge invariant actions for arbitrary conformally extended algebras.Comment: 9 page

Geometry, Isometries and Gauging of (2,1) Heterotic Sigma-Models

The geometry of (2,1) supersymmetric sigma-models is reviewed and the conditions under which they have isometry symmetries are analysed. Certain potentials are constructed that play an important role in the gauging of such symmetries. The gauged action is found for a special class of models.Comment: 12 pages, LaTeX, no figures. Minor changes; version to appear in Physics Letters

Potentials for (p,0) and (1,1) supersymmetric sigma models with torsion

Using (1,0) superfield methods, we determine the general scalar potential consistent with off-shell (p,0) supersymmetry and (1,1) supersymmetry in two-dimensional non-linear sigma models with torsion. We also present an extended superfield formulation of the (p,0) models and show how the (1,1) models can be obtained from the (1,1)-superspace formulation of the gauged, but massless, (1,1) sigma model.Comment: 11 page

Flux Compactifications of String Theory on Twisted Tori

Global aspects of Scherk-Schwarz dimensional reduction are discussed and it is shown that it can usually be viewed as arising from a compactification on the compact space obtained by identifying a (possibly non-compact) group manifold G under a discrete subgroup Gamma, followed by a truncation. This allows a generalisation of Scherk-Schwarz reductions to string theory or M-theory as compactifications on G/Gamma, but only in those cases in which there is a suitable discrete subgroup of G. We analyse such compactifications with flux and investigate the gauge symmetry and its spontaneous breaking. We discuss the covariance under O(d,d), where d is the dimension of the group G, and the relation to reductions with duality twists. The compactified theories promote a subgroup of the O(d,d) that would arise from a toroidal reduction to a gauge symmetry, and we discuss the interplay between the gauge symmetry and the O(d,d,Z) T-duality group, suggesting the role that T-duality should play in such compactifications.Comment: 43 page

Sleepless in Syracuse: Plato and the Nocturnal Council

I defend the Seventh Letter, traditionally attributed to Plato, against Michael Frede's argument that it presents a political philosophy inconsistent with that found in the Laws. Frede argues that Plato had given up the idea of the philosopher-king in his Laws, but the 7th Letter seems to be still committed to the project. I argue the Laws, particularly with the introduction of the Nocturnal Council, has Philosopher-Rulers in all but name. I consider the education of the Nocturnal Council and how it functions relative to the other constitutional structures of Magnesia. Frede advances several other arguments that the 7th Letter is spurious, but it at least escapes the most damning charge that it is inconsistent with the Laws philosophically

The Non-Perturbative SO(32) Heterotic String

The SO(32) heterotic string can be obtained from the type IIB string by gauging a discrete symmetry that acts as $(-1)^{F_L}$ on the perturbative string states and reverses the parity of the D-string. Consistency requires the presence of 32 NS 9-branes -- the S-duals of D9-branes -- which give SO(32) Chan-Paton factors to open D-strings. At finite string coupling, there are SO(32) charges tethered to the heterotic string world-sheet by open D-strings. At zero-coupling, the D-string tension becomes infinite and the SO(32) charges are pulled onto the world-sheet, and give the usual SO(32) world-sheet currents of the heterotic string.Comment: 12 Pages, Tex, Phyzzx Macr