2009
DOI: 10.1007/s00208-009-0397-6
|View full text |Cite|
|
Sign up to set email alerts
|

Deformation-obstruction theory for complexes via Atiyah and Kodaira–Spencer classes

Abstract: Abstract. We give a universal approach to the deformation-obstruction theory of objects of the derived category of coherent sheaves over a smooth projective family. We recover and generalise the obstruction class of Lowen and Lieblich, and prove that it is a product of Atiyah and Kodaira-Spencer classes. This allows us to obtain deformation-invariant virtual cycles on moduli spaces of objects of the derived category on threefolds.

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
2
1

Citation Types

1
192
0

Year Published

2009
2009
2022
2022

Publication Types

Select...
5
4

Relationship

2
7

Authors

Journals

citations
Cited by 126 publications
(193 citation statements)
references
References 22 publications
1
192
0
Order By: Relevance
“…obtained as in Example 2.1, the theorem can also be deduced from the more general results in [22]. (The assumptions on the non-positive Ext's are not needed in [22].) Our main application of this theorem concerns the case where E n is a Fourier-Mukai kernel.…”
Section: Deformation Of the Fourier-mukai Kernelmentioning
confidence: 92%
See 1 more Smart Citation
“…obtained as in Example 2.1, the theorem can also be deduced from the more general results in [22]. (The assumptions on the non-positive Ext's are not needed in [22].) Our main application of this theorem concerns the case where E n is a Fourier-Mukai kernel.…”
Section: Deformation Of the Fourier-mukai Kernelmentioning
confidence: 92%
“…When the deformation X n is integrable, e.g. obtained as in Example 2.1, the theorem can also be deduced from the more general results in [22]. (The assumptions on the non-positive Ext's are not needed in [22].)…”
Section: Deformation Of the Fourier-mukai Kernelmentioning
confidence: 99%
“…is shown in [26,13] to define a perfect obstruction theory for P n (X, β) of virtual dimension zero. A virtual cycle is then obtained by [4,22].…”
Section: Introductionmentioning
confidence: 99%
“…X is a Calabi-Yau threefold, MNOP and stable pair invariants take a particularly simple form. Then the virtual dimension is zero and we get invariants by taking the length of the 0-dimensional virtual cycle: In this case the deformation-obstruction theories [24,21,9] used to define the virtual cycles are self dual in the sense of [2]. This implies that I .…”
Section: Introductionmentioning
confidence: 99%