In algebraic geometry, given a Deligne–Mumford stack X, a perfect obstruction theory for X consists of:
E=[E-1\toE0]
D(Qcoh(X)et)
\varphi\colonE\tobf{L}X
bf{L}X
h0
h-1
The notion was introduced by for an application to the intersection theory on moduli stacks; in particular, to define a virtual fundamental class.
I\colonY\toW
\begin{matrix} X&\xrightarrow{j}&V\\ g\downarrow&&\downarrowf\\ Y&\xrightarrow{i}&W \end{matrix}
V,W
E\bullet=
\vee | |
[g | |
Y/W |
\to
*\Omega | |
j | |
V] |
-1,0
\vee | |
g | |
Y/W |
\tog*i
*\Omega | |
W |
=j*f
*\Omega | |
W |
\to
*\Omega | |
j | |
V |
\bullet | |
L | |
X |
\bullet | |
g | |
Y |
\to
\bullet | |
L | |
X |
\bullet | |
j | |
V |
\to
\bullet | |
L | |
X |
[X,E\bullet]=i![V]
Consider a smooth projective variety
Y\subsetPn
V=W
D[-1,0](X)
\vee | |
[N | |
X/Pn |
\to
\Omega | |
Pn |
]
[X,E\bullet]=i![Pn]
Y
The previous construction works too with Deligne–Mumford stacks.
By definition, a symmetric obstruction theory is a perfect obstruction theory together with nondegenerate symmetric bilinear form.
Example: Let f be a regular function on a smooth variety (or stack). Then the set of critical points of f carries a symmetric obstruction theory in a canonical way.
Example: Let M be a complex symplectic manifold. Then the (scheme-theoretic) intersection of Lagrangian submanifolds of M carries a canonical symmetric obstruction theory.