F-theory and Orientifolds
Ashoke Sen
TL;DR
This work analyzes $F$-theory on $K3$ near the orbifold limit and demonstrates its equivalence to a Type IIB orientifold on $T^2$, which via T-duality connects to Type I on $T^2$ and to heterotic on $T^2$. Away from the orbifold point, non-perturbative effects split an orientifold plane and induce non-trivial $SL(2,\mathbb{Z})$ monodromy, yielding a Seiberg-Witten–like structure in which enhanced gauge symmetries in the orientifold/$F$-theory precisely mirror enhanced global symmetries in the Seiberg-Witten theory for $SU(2)$ with four flavors. The analysis establishes a one-to-one correspondence between points of enhanced gauge symmetry in the orientifold/$F$-theory and points of enhanced global symmetry in the Seiberg-Witten setup, and it shows how the BPS spectrum can be captured by period integrals of the holomorphic two-form on the $F$-theory geometry. The work further demonstrates a triality action that links SL(2,$\mathbb{Z}$) duality to representations of $SO(8)$ and clarifies non-perturbative corrections through a dual heterotic description, strengthening the web of dualities among $F$-theory, orientifolds, Type I, and heterotic strings.
Abstract
By analyzing $F$-theory on $K3$ near the orbifold limit of $K3$ we establish the equivalence between $F$-theory on $K3$ and an orientifold of type IIB on $T^2$, which in turn, is related by a T-duality transformation to type I theory on $T^2$. By analyzing the $F$-theory background away from the orbifold limit, we show that non-perturbative effects in the orientifold theory splits an orientifold plane into two planes, with non-trivial SL(2,Z) monodromy around each of them. The mathematical description of this phenomenon is identical to the Seiberg-Witten result for N=2 supersymmetric $SU(2)$ gauge theory with four quark flavors. Points of enhanced gauge symmetry in the orientifold / $F$-theory are in one to one correspondence with the points of enhanced global symmetry in the Seiberg-Witten theory.
