2011
DOI: 10.1215/00127094-1444249
|View full text |Cite
|
Sign up to set email alerts
|

The space of stability conditions on the local projective plane

Abstract: ABSTRACT. We study the space of stability conditions on the total space of the canonical bundle over the projective plane. We explicitly describe a chamber of geometric stability conditions, and show that its translates via autoequivalences cover a whole connected component. We prove that this connected component is simply-connected. We determine the group of autoequivalences preserving this connected component.Finally, we show that there is a submanifold isomorphic to the universal covering of a moduli space … Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

2
125
0

Year Published

2013
2013
2019
2019

Publication Types

Select...
4
3

Relationship

4
3

Authors

Journals

citations
Cited by 90 publications
(127 citation statements)
references
References 50 publications
2
125
0
Order By: Relevance
“…Therefore We now investigate the limiting point lim t→+0 σ t of the above weak stability conditions. The following lemma shows that the one parameter family in Lemma 4.13 connects the 'large volume limit point' with the 'orbifold point', a similar picture obtained by Bayer-Macri [BM11] for the space of Bridgeland stability conditions on local P 2 (cf. Figure 1 in Subsection 1.4).…”
Section: Definition 412 ([Tod10a])supporting
confidence: 64%
See 1 more Smart Citation
“…Therefore We now investigate the limiting point lim t→+0 σ t of the above weak stability conditions. The following lemma shows that the one parameter family in Lemma 4.13 connects the 'large volume limit point' with the 'orbifold point', a similar picture obtained by Bayer-Macri [BM11] for the space of Bridgeland stability conditions on local P 2 (cf. Figure 1 in Subsection 1.4).…”
Section: Definition 412 ([Tod10a])supporting
confidence: 64%
“…The proof of Theorem 1.2 follows from wall-crossing argument in the space of weak stability conditions, as in the author's previous papers [Tod10a], [Tod13], [Tod12]. In order to explain the argument, we first recall Bayer-Macri's description of the space Stab(ω P 2 ) of Bridgeland stability conditions on D b Coh(ω P 2 ) in [BM11]. They showed that the double quotient stack of Stab(ω P 2 ) by the actions of Aut D b Coh(ω P 2 ) and the additive group C contains the parameter space of the mirror family of ω P 2 .…”
mentioning
confidence: 99%
“…This notion is equivalent to σ being "full" in the sense of [14], see [10,Proposition 12.4]. The definition is quite natural: it implies that if W is in an -neighborhood of Z with respect to the operator norm on Hom( R , C) induced by and the standard norm on C, then W (E) is in a disc of radius C |Z (E)| around Z (E) for all semistable objects E; in particular, we can bound the difference of the arguments of the complex numbers Z (E) and W (E).…”
Section: Equivalent Definitions Of the Support Propertymentioning
confidence: 99%
“…The main result is the following (see [Bri08,AB13,BM11]). We will choose Λ = K num (X) and v as the Chern character map as in Example 5.7.…”
Section: Stability Conditions On Surfacesmentioning
confidence: 89%
“…Arcara and Bertram realized that the construction can be generalized to any surface by using the Bogomolov Inequality in [AB13]. The proof of the support property is in [BM11,BMT14,BMS14]. As a consequence, these stability conditions vary continuously in ω and B.…”
Section: Introductionmentioning
confidence: 99%