The map between the moduli space of F-theory (or type II string) compactifications and heterotic string compactifications can be considerably simplified by using "stable degenerations". We discuss how this method applies to both the E8 x E8 and the Spin(32)/Z2 heterotic string. As a simple application of this method we derive some basic properties of the nonperturbative physics of collections of E8 or Spin(32)/Z2 point-like instantons sitting at A-D-E singularities on a K3 surface
We examine how to construct explict heterotic string models dual to F-theory in eight dimensions. In...
We study the duality between four-dimensional $\mathcal{N}$ = 2 compactifications of heterotic and ...
We give a detailed account on heterotic E8 x E8 orbifold models with N=(1,0), D=6 supersymmetry usin...
We consider the compactification of the E8xE8 heterotic string on a K3 surface with "the spin connec...
Abstract By fibering the duality between the E 8 × E 8 heterotic string on T 3 and M-theory on K3, w...
We study F-theory duals of six dimensional heterotic vacua in extreme regions of moduli space where ...
The subspace of the moduli space of F-theory on K3 over which the coupling remains constant develops...
We discuss N=2 supersymmetric compactifications to four dimensions from the point of view of F-theor...
By analyzing F-theory on K3 near the orbifold limit of K3 we establish the equivalence between F-the...
By analyzing F-theory on K3 near the orbifold limit of K3 we establish the equivalence between F-the...
A while ago, examples of N=1 vacua in D=6 were constructed as orientifolds of Type IIB string theory...
Compactifications of the heterotic string on T^d are the simplest, yet rich enough playgrounds to un...
We analyze the map between heterotic and type II N=2 supersymmetric string theories for certain two ...
Eight-dimensional non-geometric heterotic strings with gauge algebra $\mathfrak{e}_8\mathfrak{e}_7$ ...
We study a class of 6d $\mathcal{N}=(1,0)$ non-geometric vacua of the $\text{Spin}(32)/\mathbb Z_2$ ...
We examine how to construct explict heterotic string models dual to F-theory in eight dimensions. In...
We study the duality between four-dimensional $\mathcal{N}$ = 2 compactifications of heterotic and ...
We give a detailed account on heterotic E8 x E8 orbifold models with N=(1,0), D=6 supersymmetry usin...
We consider the compactification of the E8xE8 heterotic string on a K3 surface with "the spin connec...
Abstract By fibering the duality between the E 8 × E 8 heterotic string on T 3 and M-theory on K3, w...
We study F-theory duals of six dimensional heterotic vacua in extreme regions of moduli space where ...
The subspace of the moduli space of F-theory on K3 over which the coupling remains constant develops...
We discuss N=2 supersymmetric compactifications to four dimensions from the point of view of F-theor...
By analyzing F-theory on K3 near the orbifold limit of K3 we establish the equivalence between F-the...
By analyzing F-theory on K3 near the orbifold limit of K3 we establish the equivalence between F-the...
A while ago, examples of N=1 vacua in D=6 were constructed as orientifolds of Type IIB string theory...
Compactifications of the heterotic string on T^d are the simplest, yet rich enough playgrounds to un...
We analyze the map between heterotic and type II N=2 supersymmetric string theories for certain two ...
Eight-dimensional non-geometric heterotic strings with gauge algebra $\mathfrak{e}_8\mathfrak{e}_7$ ...
We study a class of 6d $\mathcal{N}=(1,0)$ non-geometric vacua of the $\text{Spin}(32)/\mathbb Z_2$ ...
We examine how to construct explict heterotic string models dual to F-theory in eight dimensions. In...
We study the duality between four-dimensional $\mathcal{N}$ = 2 compactifications of heterotic and ...
We give a detailed account on heterotic E8 x E8 orbifold models with N=(1,0), D=6 supersymmetry usin...