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Torus Knots and Minimal Models Revisited : Rational VOA characters from non-hyperbolic knots

Dongmin Gang, Byoungyoon Park, Huijoon Sohn

TL;DR

The paper develops a physical framework uniting the Hikami–Kirillov link between torus knots and Virasoro minimal models with the 3D–3D correspondence and a bulk–boundary dictionary. By analyzing 3D ${ m N}=2$ theories $T[S^3ackslash { m K}_{(P,Q)}]$ via Dimofte–Gaiotto–Gukov data and a bulk-twisted boundary construction, it shows that IR phases realize either unitary TQFTs or rank-0 ${ m N}=4$ SCFTs, whose twisted sectors yield rational VOAs at the boundary. The work provides explicit Nahm-sum–like expressions and half-indices for Virasoro and related rational CFT characters directly from ideal triangulations, along with extensive examples for torus knots $(P,Q)=(2,5),(2,7),(5,7)$, etc. It also discusses decoupling of $U(1)_m$ in the IR, reduction to simpler UV descriptions, and the interpretation of boundary VOAs via A/B twists and parity. This framework offers a systematic route to construct and identify boundary RCFT characters from combinatorial knot data and suggests broad generalizations to higher rank theories and other non-hyperbolic manifolds with potential Haagerup-like RCFTs.

Abstract

In 2003, Hikami and Kirillov uncovered an intriguing connection between torus knots $\mathcal{K}_{(P,Q)}$ and Virasoro minimal models $\mathcal{M}(P,Q)$ by relating the Kashaev invariants of the knots to the characters of the corresponding minimal models. In this work, we recover and extend this connection by combining the 3D--3D correspondence with a bulk--boundary correspondence. More concretely, we study the 3D $\mathcal{N}=2$ gauge theories associated with torus-knot complements via the Dimofte--Gaiotto--Gukov construction and show that, in the infrared, these theories either flow to a unitary TQFT (when $|P-Q| = 1$), whose boundary chiral algebra reproduces that of the associated unitary minimal model, or to a 3D $\mathcal{N}=4$ rank-0 SCFT (when $|P-Q| > 1$), which realizes the corresponding non-unitary chiral minimal model at the boundary after an appropriate topological twist. This framework yields new Nahm-sum-like expressions for the characters of Virasoro minimal models and other related rational conformal field theories, providing a systematic algorithm for constructing characters of rational VOAs directly from the combinatorial data of an ideal triangulation of a non-hyperbolic knot complement.

Torus Knots and Minimal Models Revisited : Rational VOA characters from non-hyperbolic knots

TL;DR

The paper develops a physical framework uniting the Hikami–Kirillov link between torus knots and Virasoro minimal models with the 3D–3D correspondence and a bulk–boundary dictionary. By analyzing 3D theories via Dimofte–Gaiotto–Gukov data and a bulk-twisted boundary construction, it shows that IR phases realize either unitary TQFTs or rank-0 SCFTs, whose twisted sectors yield rational VOAs at the boundary. The work provides explicit Nahm-sum–like expressions and half-indices for Virasoro and related rational CFT characters directly from ideal triangulations, along with extensive examples for torus knots , etc. It also discusses decoupling of in the IR, reduction to simpler UV descriptions, and the interpretation of boundary VOAs via A/B twists and parity. This framework offers a systematic route to construct and identify boundary RCFT characters from combinatorial knot data and suggests broad generalizations to higher rank theories and other non-hyperbolic manifolds with potential Haagerup-like RCFTs.

Abstract

In 2003, Hikami and Kirillov uncovered an intriguing connection between torus knots and Virasoro minimal models by relating the Kashaev invariants of the knots to the characters of the corresponding minimal models. In this work, we recover and extend this connection by combining the 3D--3D correspondence with a bulk--boundary correspondence. More concretely, we study the 3D gauge theories associated with torus-knot complements via the Dimofte--Gaiotto--Gukov construction and show that, in the infrared, these theories either flow to a unitary TQFT (when ), whose boundary chiral algebra reproduces that of the associated unitary minimal model, or to a 3D rank-0 SCFT (when ), which realizes the corresponding non-unitary chiral minimal model at the boundary after an appropriate topological twist. This framework yields new Nahm-sum-like expressions for the characters of Virasoro minimal models and other related rational conformal field theories, providing a systematic algorithm for constructing characters of rational VOAs directly from the combinatorial data of an ideal triangulation of a non-hyperbolic knot complement.
Paper Structure (122 sections, 531 equations, 3 figures)

This paper contains 122 sections, 531 equations, 3 figures.

Figures (3)

  • Figure 1: Schematic summary of the main proposal of this work. The 3D $\mathcal{N}=2$ supersymmetric gauge theory $T[S^{3}\backslash \mathcal{K}_{(P,Q)}]$, associated with a torus-knot complement via the 3D--3D correspondence, exhibits two distinct infrared behaviors. For $|P-Q|=1$, the theory flows to a unitary TQFT, whereas for $|P-Q|>1$ it flows to a three-dimensional $\mathcal{N}=4$ rank-$0$ superconformal field theory. The subsequent bulk--boundary correspondence then realizes, depending on the choice of boundary conditions, the rational vertex operator algebra of the corresponding Virasoro minimal model $\mathcal{M}(P,Q)$ or other closely related rational conformal field theories at the boundary.
  • Figure 2: Schematic summary of the construction of r-VOA characters from the combinatorial data of an ideal triangulation of $S^3\backslash \mathcal{K}_{(P,Q)}$.
  • Figure 3: Absolute value of the round $S^3$ partition function for $T[S^3\backslash {\cal K}_{(P,Q)=(2,7)}]$, computed using the Bethe-sum formula in \ref{['Bethe-sum for S3']}. The partition function attains its minimum at $\nu=\nu_{\rm con}=1$, where the value is $\frac{2}{\sqrt{7}}\sin\!(\frac{6\pi}{7}) \approx 0.327985$. At $\nu=0$, the value $\frac{2}{\sqrt{7}}\sin\!(\frac{2\pi}{7}) \approx 0.591009$ matches $|S_{00}|$ of the minimal model ${\cal M}(2,7)$. At $\nu=2$, the value is $\frac{2}{\sqrt{7}}\sin\!(\frac{4\pi}{7}) \approx 0.736976$.