Three-Dimensional Quantum Gravity, Chern-Simons Theory, and the A-Polynomial
By Sergei Gukov. 2003
334 citations recorded by the source corpus.
We study three-dimensional Chern-Simons theory with complex gauge group SL(2,ℂ), which has many interesting connections with three-dimensional quantum gravity and geometry of hyperbolic 3-manifolds. We show that, in the presence of a single knotted Wilson loop in an infinite-dimensional representation of the gauge group, the classical and quantum properties of such theory are described by an algebraic curve called the A-polynomial of a knot. Using this approach, we find some new and rather surprising relations between the A-polynomial, the colored Jones polynomial, and other invariants of hyperbolic 3-manifolds. These relations generalize the volume conjecture and the Melvin-Morton-Rozansky conjecture, and suggest an intriguing connection between the SL(2,ℂ) partition function and the colored Jones polynomial.
Subfields: Geometry and Topology, Nuclear and High Energy Physics
View Paper: https://www.semanticscholar.org/paper/debec40e9e09ee932a3f238d1cff08bbf39c050c
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Citations in the corpus
- 3-Manifolds and 3d Indices (2011, background): “quot;) edge. Otherwise, it has been proven that all hyperbolic knot complements have non-univalent triangulations [58], and the same seems to hold even for non-hyperbolic knots [56]. { 27 { (see e.g. [28]): P @M = C C Z 2 = f(‘;m)g (‘;m) ˘(‘ 1;m 1) : (4.14) Finally, we take the canonical position ”
- Generalized volume conjecture and the A-polynomials: The Neumann–Zagier potential function as a classical limit of the partition function (2006, background): “…is conjectured to dominate the asymptotics of the invariant J K N; e 2πi/N in the large-N limit N → ∞, lim N→∞ 2 π N log J K N; e 2πi/N = Vol(S 3 \ K) (1.1) This " volume conjecture " is generalized for other values (near the N-th root of unity) of the Ncolored Jones polynomial [18] (see also Refs.”
- A-polynomial, B-model, and quantization (2011, methodology): “,C) Chern-Simons theory with a Wilson loop, the polynomial A(x,y) is a topological invariant called the A-polynomial and plays a role similar to that of the Seiberg-Witten curve in N = 2 gauge theory [3]. The parameter ~is the coupling constant of Chern-Simons theory. 3. Matrix models: In matrix mod”
- 6j–symbols, hyperbolic structures and the volume conjecture (2006, methodology): “In [ 10 ], S. Gukov proposed the following generalization of the Volume Conjecture for hyperbolic knots in S3:”
- On dualizability of braided tensor categories (2018, background): “As such, it should provide a foundational framework for: quantum A-polynomials [Dim13, Gar04, Guk05, GS12], DAHAJones polynomials and skein modules of knots complements [Che13, BS16, Sam17], and refined Chern–Simons invariants [AS15], among others, each of which yet lacks a topologically invariant f”
- Fivebranes and 4-manifolds (2013, background): “slightly more interesting theory φai ◦T[S1 ×D2], whose space of supersymetric vacua (2.12) is simply an SL(2,Z) transform of (2.44): Vφ ai◦T[S1×D2] = ˆ (xi,yi) ∈ TC×TC W ixa i yi= 1 ˙ (2.45) See e.g. [42] for more details on Dehn surgery in the context of complex Chern-Simons theory. The space of va”
- Chern-Simons theory, analytic continuation and arithmetic (2007, background): “p τK,G(z) = L p K,G(−z). Unlike the case of Conjecture 2, this is an easy corollary of its very definition. Remark 1.3. Chern-Simons theory with complex gauge group was studied extensively by Gukov in [Gu]. It is an interesting problem to compare forthcoming work of Gukov-Zagier on modularity propert”
- The colored Jones polynomials of the figure-eight knot and its Dehn surgery spaces (2004, methodology): “ith E the figure-eight knot. Then it turns out that it determines the potential function introduced by W. Neumann and D. Zagier [16] to study the volumes of Dehn surgered spaces along knots. (See also [1].) The we apply T. Yoshida’s theorem [24] to show that the limit of log JN E;exp(2πr √ −1/N) /N”
- Exact results for perturbative Chern-Simons theory with complex gauge group. (2009, background): “Every such M can be represented as a quotient M = H3/Γ (2.6) of the hyperbolic space H3 by a discrete, torsion-free subgroup Γ ⊂ PSL(2,C), which is a holonomy representation of the fundamental group π1(M) into Isom +(H3) = PSL(2,C).”
- Quantum foam and topological strings (2003, background): “space of connections is an enlargement of the space of allowed metrics [11] (see [ 17 ] for”
- Gauge Theories Labelled by Three-Manifolds (2011, background): “nections on @Mg (gauge equivalence): (2.1) 1The equivalence between at connections and hyperbolic geometry results from the fact that the isometry group of hyperbolic three-space is (P)SL(2;C), cf. [6, 7, 8, 9]. Almost all at connections can be realized as (possibly degenerate) hyperbolic metrics; ”
- Non semi-simple TQFTs, Reidemeister torsion and Kashaev's invariants (2014, neutral): “ C. BLANCHET, F. COSTANTINO, N. GEER, AND B. PATUREAU-MIRAND Lemma A.5 (General hopf links). 8i;j2f0;1;:::;r 2gand 8;2C, one has V d;V f = ( r1) 1r ( ) q Id V S i;S j = ( 1) i f(i+ 1)(j+ 1)g j+ 1g (35) Id V j S i;V = f(i+ 1)g fg Id V d P i;V = ( 1) r 1r q (r 1 i) + q (r 1 i) ( ) (36) Id V S i;P j = ”
- Quantum Riemann Surfaces in Chern-Simons Theory (2011, background): “ere A M(‘;m) is the so-called A-polynomial of M[3]. This condition cuts out a Lagrangian submanifold L M = fA M(‘;m) = 0g ˆ P T2 = f(‘;m)gˇC C ; (1.4) or a semi-classical state in Chern-Simons theory [4]. We would like to quantize the A-polynomial, promoting it to an operator A^ M(^‘; m^;q) that ann”