Bridgeland stability condition
In mathematics, and especially algebraic geometry, a Bridgeland stability condition, defined by Tom Bridgeland, is an algebro-geometric stability condition defined on elements of a triangulated category. The case of original interest and particular importance is when this derived category is the derived category of coherent sheaves on a Calabi–Yau manifold, and this situation has fundamental links to string theory and the study of D-branes.
Such stability conditions were introduced in a rudimentary form by Michael Douglas called -stability and used to study BPS B-branes in string theory.[1] This concept was made precise by Bridgeland, who phrased these stability conditions categorically, and initiated their study mathematically.[2]
Definition[]
The definitions in this section are presented as in the original paper of Bridgeland, for arbitrary triangulated categories.[2] Let be a triangulated category. A slicing of is a collection of full additive subcategories for each such that
- for all , where is the shift functor on the triangulated category,
- if and and , then , and
- for every object there exists a finite sequence of real numbers and a collection of triangles
- with for all .
The last property should be viewed as axiomatically imposing the existence of Harder–Narasimhan filtrations on elements of the category .
A Bridgeland stability condition on a triangulated category is a pair consisting of a slicing and a group homomorphism , where is the Grothendieck group of , called a central charge, satisfying
- if then for some strictly positive real number .
It is convention to assume the category is essentially small, so that the collection of all stability conditions on forms a set . In good circumstances, for example when is the derived category of coherent sheaves on a complex manifold , this set actually has the structure of a complex manifold itself.
It is shown by Bridgeland that the data of a Bridgeland stability condition is equivalent to specifying a bounded t-structure on the category and a central charge on the heart of this t-structure which satisfies the Harder–Narasimhan property above.[2] An element is semi-stable (resp. stable) with respect to the stability condition if for every surjection for , we have where and similarly for .
References[]
- Geometry
- String theory
- Algebraic geometry