2011
DOI: 10.1016/j.nuclphysb.2011.03.014
|View full text |Cite
|
Sign up to set email alerts
|

The volume conjecture, perturbative knot invariants, and recursion relations for topological strings

Abstract: We study the relation between perturbative knot invariants and the free energies defined by topological string theory on the character variety of the knot. Such a correspondence between SL(2; C) Chern-Simons gauge theory and the topological open string theory was proposed earlier on the basis of the volume conjecture and AJ conjecture. In this paper we discuss this correspondence beyond the subleading order in the perturbative expansion on both sides. In the computation of the perturbative invariants for the h… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

8
108
0
8

Year Published

2012
2012
2017
2017

Publication Types

Select...
4
3

Relationship

0
7

Authors

Journals

citations
Cited by 94 publications
(138 citation statements)
references
References 76 publications
8
108
0
8
Order By: Relevance
“…(2.7) differs from that in [16]. As will be explained below, these differences are important for overcoming the obstacles in [16] and reproducing the "quantum" q-corrections in the quantization of the A-polynomial (2.1).…”
Section: Jhep02(2012)070mentioning
confidence: 97%
See 2 more Smart Citations
“…(2.7) differs from that in [16]. As will be explained below, these differences are important for overcoming the obstacles in [16] and reproducing the "quantum" q-corrections in the quantization of the A-polynomial (2.1).…”
Section: Jhep02(2012)070mentioning
confidence: 97%
“…We plan to elucidate the relation between these two properties in the future work. 16 At first, this may seem a little surprising, because the quantization problem is about symplectic geometry and not about complex geometry of C. (Figuratively speaking, quantization aims to replace all classical objects in symplectic geometry by the corresponding quantum analogs.) However, our "phase space," be it C × C or C * × C * , is very special in a sense that it comes equipped with a whole CP 1 worth of complex and symplectic structures, so that each aspect of the geometry can be looked at in several different ways, depending on which complex or symplectic structure we choose.…”
Section: Relation To Algebraic K-theorymentioning
confidence: 99%
See 1 more Smart Citation
“…. ), and has appeared provably or experimentally in many problems of 2D enumerative geometry: the two hermitian matrix model [EO08] and the chain of hermitian matrices [CEO06], topological string theory and Gromov-Witten invariants [BKMP09, BEMS10, EMS09, MP12, NS11, EO12], integrable systems [BE09,BE10,BE11], intersection numbers on the moduli space of curves [EO07b,Eyn11b,Eyn11a], asymptotic of knot invariants [DFM11,BE12,BEM12], . .…”
Section: Problem and Main Resultsmentioning
confidence: 99%
“…This has been achieved for the torus knots [101,102]. There are still difficulties implementing AMM/EO topological recursion for twist knots [103,104] but there is some evidence of applicability of AMM/EO recursion to the non-torus knot 4 1 [105].…”
Section: Jhep08(2017)139mentioning
confidence: 97%