2012
DOI: 10.1007/s00029-011-0081-z
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Motivic invariants of quivers via dimensional reduction

Abstract: We provide a reduction formula for the motivic Donaldson-Thomas invariants associated to a quiver with superpotential. The method is valid provided the superpotential has a linear factor, it allows us to compute virtual motives in terms of ordinary motivic classes of simpler quiver varieties. We outline an application, giving explicit formulas for the motivic Donaldson-Thomas invariants of the orbifolds [C × C 2 /Zn].

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Cited by 13 publications
(29 citation statements)
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References 17 publications
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“…Using these formulas, absence of exotics for framed and unframed invariants reduces to absence of exotics for the framed asymptotic ones. The latter will then be proven shortly using the results of [116]. Therefore, in short, rationality of both framed and unframed invariants is established, granting the motivic wallcrossing formula of [106] for SU (N ) quivers.…”
Section: 5mentioning
confidence: 78%
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“…Using these formulas, absence of exotics for framed and unframed invariants reduces to absence of exotics for the framed asymptotic ones. The latter will then be proven shortly using the results of [116]. Therefore, in short, rationality of both framed and unframed invariants is established, granting the motivic wallcrossing formula of [106] for SU (N ) quivers.…”
Section: 5mentioning
confidence: 78%
“…Motivic NCDT invariants can also be explicitly computed in certain examples using different techniques [130,121,117,118,116]. A computation based on [116] is outlined for SU (N ) quivers in Section 7.5.…”
Section: 4mentioning
confidence: 99%
“…The cyclic quiver. The proof of Theorem 3.6 proceeds analogously to the conifold case, using dimensional reduction and appropriate splittings, reducing the calculation to the case q = 1 already done in [9,24]. Once again, we refer for the details to [10].…”
Section: 4mentioning
confidence: 99%
“…The results we are reporting on here are rather limited. In particular, we do not introduce any new techniques for computing DT invariants in this paper; rather we use the dimensional reduction technique already used in [6], and systematized in [24], to see what we can learn about the structure of the invariants and their deformation properties. Thus, the cases in which we have been able to compute the generating series for the motivic DT invariants are the cases in which the potential is linear with respect to one of the generators of the algebra.…”
Section: Introductionmentioning
confidence: 99%
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