Bridgeland Stability Condition
   HOME

TheInfoList



OR:

In
mathematics Mathematics is a field of study that discovers and organizes methods, Mathematical theory, theories and theorems that are developed and Mathematical proof, proved for the needs of empirical sciences and mathematics itself. There are many ar ...
, and especially
algebraic geometry Algebraic geometry is a branch of mathematics which uses abstract algebraic techniques, mainly from commutative algebra, to solve geometry, geometrical problems. Classically, it studies zero of a function, zeros of multivariate polynomials; th ...
, a Bridgeland stability condition, defined by Tom Bridgeland, is an algebro-geometric stability condition defined on elements of a
triangulated category In mathematics, a triangulated category is a category with the additional structure of a "translation functor" and a class of "exact triangles". Prominent examples are the derived category of an abelian category, as well as the stable homotopy ca ...
. The case of original interest and particular importance is when this triangulated category is the
derived category In mathematics, the derived category ''D''(''A'') of an abelian category ''A'' is a construction of homological algebra introduced to refine and in a certain sense to simplify the theory of derived functors defined on ''A''. The construction pr ...
of
coherent sheaves In mathematics, especially in algebraic geometry and the theory of complex manifolds, coherent sheaves are a class of sheaves closely linked to the geometric properties of the underlying space. The definition of coherent sheaves is made with refer ...
on a
Calabi–Yau manifold In algebraic and differential geometry, a Calabi–Yau manifold, also known as a Calabi–Yau space, is a particular type of manifold which has certain properties, such as Ricci flatness, yielding applications in theoretical physics. P ...
, and this situation has fundamental links to
string theory In physics, string theory is a theoretical framework in which the point-like particles of particle physics are replaced by one-dimensional objects called strings. String theory describes how these strings propagate through space and intera ...
and the study of
D-brane In string theory, D-branes, short for Dirichlet membrane, are a class of extended objects upon which open strings can end with Dirichlet boundary conditions, after which they are named. D-branes are typically classified by their spatial dimensi ...
s. Such stability conditions were introduced in a rudimentary form by
Michael Douglas Michael Kirk Douglas (born September 25, 1944) is an American actor and film producer. He has received numerous accolades, including two Academy Awards, five Golden Globe Awards, a Primetime Emmy Award, the Cecil B. DeMille Award, and the ...
called \Pi-stability and used to study BPS B-branes in string theory.Douglas, M.R., Fiol, B. and Römelsberger, C., 2005. Stability and BPS branes. Journal of High Energy Physics, 2005(09), p. 006. This concept was made precise by Bridgeland, who phrased these stability conditions categorically, and initiated their study mathematically.


Definition

The definitions in this section are presented as in the original paper of Bridgeland, for arbitrary triangulated categories. Let \mathcal be a triangulated category.


Slicing of triangulated categories

A slicing \mathcal of \mathcal is a collection of full additive subcategories \mathcal(\varphi) for each \varphi\in \mathbb such that * \mathcal(\varphi) = \mathcal(\varphi+1) for all \varphi, where /math> is the shift functor on the triangulated category, * if \varphi_1 > \varphi_2 and A\in \mathcal(\varphi_1) and B\in \mathcal(\varphi_2), then \operatorname(A,B)=0, and * for every object E\in \mathcal there exists a finite sequence of real numbers \varphi_1>\varphi_2>\cdots>\varphi_n and a collection of triangles ::: :with A_i\in \mathcal(\varphi_i) for all i. The last property should be viewed as axiomatically imposing the existence of Harder–Narasimhan filtrations on elements of the category \mathcal.


Stability conditions

A Bridgeland stability condition on a triangulated category \mathcal is a pair (Z,\mathcal) consisting of a slicing \mathcal and a group homomorphism Z: K(\mathcal) \to \mathbb, where K(\mathcal) is the
Grothendieck group In mathematics, the Grothendieck group, or group of differences, of a commutative monoid is a certain abelian group. This abelian group is constructed from in the most universal way, in the sense that any abelian group containing a group homomorp ...
of \mathcal, called a central charge, satisfying * if 0\ne E\in \mathcal(\varphi) then Z(E) = m(E) \exp(i\pi \varphi) for some strictly positive real number m(E) \in \mathbb_. It is convention to assume the category \mathcal is essentially small, so that the collection of all stability conditions on \mathcal forms a set \operatorname(\mathcal). In good circumstances, for example when \mathcal = \mathcal^b \operatorname(X) is the derived category of coherent sheaves on a complex manifold X, this set actually has the structure of a complex manifold itself.


Technical remarks about stability condition

It is shown by Bridgeland that the data of a Bridgeland stability condition is equivalent to specifying a bounded
t-structure In the branch of mathematics called homological algebra, a ''t''-structure is a way to axiomatize the properties of an abelian subcategory of a derived category. A ''t''-structure on \mathcal consists of two subcategories (\mathcal^, \mathcal^) o ...
\mathcal(>0) on the category \mathcal and a central charge Z: K(\mathcal)\to \mathbb on the heart \mathcal = \mathcal((0,1]) of this t-structure which satisfies the Harder–Narasimhan property above. An element E\in\mathcal is semi-stable (resp. stable) with respect to the stability condition (Z,\mathcal) if for every surjection E \to F for F\in \mathcal, we have \varphi(E) \le (\text<) \, \varphi(F) where Z(E) = m(E) \exp(i\pi \varphi(E)) and similarly for F.


Examples


From the Harder–Narasimhan filtration

Recall the Harder–Narasimhan filtration for a smooth projective curve X implies for any coherent sheaf E there is a filtration
0 = E_0 \subset E_1 \subset \cdots \subset E_n = E
such that the factors E_j/E_ have slope \mu_i=\text/\text. Set \phi(E) = \arg(-\mathrm(E) + i \mathrm(E)) . We can extend this filtration to a bounded complex of sheaves E^\bullet by considering the filtration on the cohomology sheaves E^i = H^i(E^\bullet) i/math>. From this observation, the pair (Z,\mathcal) is a Bridgeland stability condition if the central charge and the slicing are defined to be Z(E) = - \mathrm(E) + \mathrm(E), \mathcal(\phi) = \.


Elliptic curves

There is an analysis by Bridgeland for the case of Elliptic curves. He finds there is an equivalence
\text(X)/\text(X) \cong \text^+(2,\mathbb)/\text(2,\mathbb)
where \text(X) is the set of stability conditions and \text(X) is the set of autoequivalences of the derived category D^b(X).


References


Papers

* Stability conditions on A_n singularities * Interactions between autoequivalences, stability conditions, and moduli problems {{DEFAULTSORT:Bridgeland stability condition Geometry String theory Algebraic geometry