For semisimple Lie algebra targets
For discrete group targets
For discrete 2-group targets
For Lie 2-algebra targets
For targets extending the super Poincare Lie algebra
(such as the supergravity Lie 3-algebra, the supergravity Lie 6-algebra)
Chern-Simons-supergravity
for higher abelian targets
for symplectic Lie n-algebroid targets
for the -structure on the BRST complex of the closed string:
higher dimensional Chern-Simons theory
topological AdS7/CFT6-sector
theory (physics), model (physics)
Axiomatizations
Tools
Structural phenomena
Types of quantum field thories
What is called the A-model topological string is the 2-dimensional topological conformal field theory corresponding to the Calabi–Yau category called the Fukaya category of a symplectic manifold . This is is effectively the Gromov–Witten theory of .
The A-model arose in formal physics from considerations of superstring-propagation on Calabi-Yau spaces: it may be motivated by considering the vertex operator algebra of the 2dSCFT given by the supersymmetric sigma-model with target space and then deforming it such that one of the super-Virasoro generators squares to . The resulting “topologically twisted” algebra may then be read as being the BRST complex of a TCFT.
One can also define an A-model for Landau–Ginzburg models. The category of D-branes for the corresponding open string theory is given by the Fukaya–Seidel category.
By homological mirror symmetry, the A-model is dual to the B-model.
The action functional of the A-model is that associated by AKSZ theory to a Lagrangian submanifold in a target symplectic Lie n-algebroid which is the Poisson Lie algebroid of a symplectic manifold.
See the references on Lagrangian formulation.
On coisotropic branes in symplectic target manifolds that arise by complexification of phase spaces, the boundary path integral of the A-model computes the quantization of that phase space. For details see
and
The second quantization effective background field theory defined by the perturbation series of the A-model string has been argued to be Chern-Simons theory. (Witten 92, Costello 06)
The A-model was first conceived in
An early review is in
The motivation from the point of view of string theory is reviewed for instance in
A summary of these two reviews is in
Discussion of how the A-model Lagrangian arises in AKSZ theory:
around page 19 in
section 5.3 of
Also
Discussion of how the second quantization effective field theory given by the A-model perturbation series is Chern-Simons theory is in
formalizing at least aspects of the observations in