We review free fermion, melting crystal, and matrix model representations of wall-crossing phenomena on local, toric Calabi-Yau manifolds. We consider both unrefined and refined BPS counting of closed BPS states involving D2- and D0-branes bound to a D6-brane, as well as open BPS states involving open D2-branes ending on an additional D4-brane. Appropriate limit of these constructions provides, among the others, matrix model representation of refined and unrefined topological string amplitudes
The number of BPS bound states of D-branes on a Calabi-Yau manifold depends on two sets of data, the...
We construct a free fermion and matrix model representation of refined Bogomol’nyi-Prasad-Sommerfeld...
Abstract: The number of BPS bound states of D-branes on a Calabi-Yau manifold depends on two sets of...
We review free fermion, melting crystal, and matrix model representations of wall-crossing phenomena...
We review free fermion, melting crystal, and matrix model representations of wall-crossing phenomena...
We review free fermion, melting crystal, and matrix model representations of wall-crossing phenomena...
We review free fermion, melting crystal, and matrix model representations of wall-crossing phenomena...
We describe wall-crossing for local, toric Calabi-Yau manifolds without compact four-cycles, in term...
We describe wall-crossing for local, toric Calabi-Yau manifolds without compact four-cycles, in term...
We consider wall-crossing phenomena associated to the counting of D2-branes attached to D4-branes wr...
We consider wall-crossing phenomena associated to the counting of D2-branes attached to D4-branes wr...
The number of BPS bound states of D-branes on a Calabi-Yau manifold depends on two sets of data, the...
The number of BPS bound states of D-branes on a Calabi-Yau manifold depends on two sets of data, the...
The number of BPS bound states of D-branes on a Calabi-Yau manifold depends on two sets of data, the...
We construct a free fermion and matrix model representation of refined Bogomol’nyi-Prasad-Sommerfeld...
The number of BPS bound states of D-branes on a Calabi-Yau manifold depends on two sets of data, the...
We construct a free fermion and matrix model representation of refined Bogomol’nyi-Prasad-Sommerfeld...
Abstract: The number of BPS bound states of D-branes on a Calabi-Yau manifold depends on two sets of...
We review free fermion, melting crystal, and matrix model representations of wall-crossing phenomena...
We review free fermion, melting crystal, and matrix model representations of wall-crossing phenomena...
We review free fermion, melting crystal, and matrix model representations of wall-crossing phenomena...
We review free fermion, melting crystal, and matrix model representations of wall-crossing phenomena...
We describe wall-crossing for local, toric Calabi-Yau manifolds without compact four-cycles, in term...
We describe wall-crossing for local, toric Calabi-Yau manifolds without compact four-cycles, in term...
We consider wall-crossing phenomena associated to the counting of D2-branes attached to D4-branes wr...
We consider wall-crossing phenomena associated to the counting of D2-branes attached to D4-branes wr...
The number of BPS bound states of D-branes on a Calabi-Yau manifold depends on two sets of data, the...
The number of BPS bound states of D-branes on a Calabi-Yau manifold depends on two sets of data, the...
The number of BPS bound states of D-branes on a Calabi-Yau manifold depends on two sets of data, the...
We construct a free fermion and matrix model representation of refined Bogomol’nyi-Prasad-Sommerfeld...
The number of BPS bound states of D-branes on a Calabi-Yau manifold depends on two sets of data, the...
We construct a free fermion and matrix model representation of refined Bogomol’nyi-Prasad-Sommerfeld...
Abstract: The number of BPS bound states of D-branes on a Calabi-Yau manifold depends on two sets of...