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Super Liouville theory on the torus: bootstrap and the super Virasoro minimal string

High Energy Physics - Theory · Submitted 1 Oct 2026 · 99 references

Pith's verdict: Careful, technically serious paper that completes the SVMS torus computation and builds reusable super-Liouville technology; the one soft spot — a postulated block — is disclosed and well-mitigated by numerics.

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arXiv ID2610.01909 (version 1)
Pith IDR64N2VTB, Pith's permanent record of this paper and its review
CitationBeatrix M\"uhlmann, Ioannis Tsiares, Jianming Zheng, Mukund Rangamani, Scott Collier. "Super Liouville theory on the torus: bootstrap and the super Virasoro minimal string." arXiv:2610.01909 (2026). https://pith.science/paper/R64N2VTB
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Referee report
The paper

The paper claims

The torus one-point amplitudes of all four super Virasoro minimal string theories, computed directly from the RNS worldsheet, agree with topological recursion on the spectral curves of the dual matrix integrals…

The reading

This paper completes the worldsheet-side toolkit for $N=1$ super Liouville theory on the torus and uses it to test a conjectured string/matrix-model duality. It corrects the recursive representations of the torus one-point super Virasoro blocks, identifies a new block in the odd spin structure built on a distinguished superdescendant, and constructs modular crossing kernels for all four spin structure sectors. Applying the technology to the super Virasoro minimal string, it computes the NS-sector sphere three-point and torus one-point amplitudes in all four theories ($0\mathrm{A}^{\pm}$ and $0\mathrm{B}^{\pm}$) directly from the RNS worldsheet and finds they agree with topological recursion on the dual matrix integral spectral curves. The agreement matters because it confirms the super Virasoro minimal string duality, including the momentum-independent hard-edge amplitude of the $0\mathrm{A}^-$ theory and the vanishing of the stable NS amplitudes of the $0\mathrm{B}^-$ theory.

What carries the argument

The carrying object is the distinguished level three-half superdescendant $\widetilde G_{-3/2}G_{-3/2}V_P$, whose torus one-point function is non-vanishing only in the odd spin structure ($\tilde R$) sector and behaves like that of a Virasoro primary. Superconformal Ward identities fix the three-point functions of this descendant, and its block $F^{DV}_1$ is combined with the picture changing operator to regulate the ghost zero-mode ambiguity in the $\tilde R$ sector. The technical apparatus consists of corrected Zamolodchikov-type elliptic recursion relations generating all torus one-point blocks, the eight modular $S$-kernels (six of them new) that express the blocks in the modular dual channel, and the structure constants and spectral densities of the spacelike and timelike super Liouville theories, whose modular covariance anchors the whole construction.

Extended reading notes

Core claim

The central claim is that the torus one-point amplitudes of the four super Virasoro minimal string theories, computed directly from the RNS worldsheet, equal the predictions of topological recursion on the spectral curves of the dual matrix integrals, with the simple values $A^{0\mathrm{A}+}_{1,(1|0)}=(4h_{\rm ext}-1)/48$, $A^{0\mathrm{B}+}_{1,(1|0)}=(4h_{\rm ext}-1)/24$, $A^{0\mathrm{A}-}_{1,(1|0)}=-1/16$, and $A^{0\mathrm{B}-}_{1,(1|0)}=0$, where $h_{\rm ext}=\frac18 Q^2+\frac12 P_{\rm ext}^2$. Along the way the paper establishes modular covariance of the torus one-point functions in both spacelike and timelike super Liouville theory and provides the missing modular crossing kernels. The computation hinges on a new object: the level three-half superdescendant $\widetilde G_{-3/2}G_{-3/2}V_P$, whose torus one-point function transforms like that of a Virasoro primary and is non-vanishing only in the odd spin structure; its one-point function supplies the $\tilde R$ contribution to the string amplitude through a careful treatment of the picture changing operator. The paper also identifies an exceptional zero-momentum Ramond insertion in the $0\mathrm{A}^-$ theory despite the absence of generic Ramond states, interprets it as a Ramond puncture, and matches its mixed sphere three-point amplitude to the intersection-theory prediction, taking the value unity.

Load-bearing premise

The odd spin structure block $F^{DV}_1$ that produces the non-vanishing correlator $\langle \widetilde G_{-3/2}G_{-3/2}V\rangle_1$ is assumed rather than derived: the authors write that they 'can simply postulate that it is given by the even elliptic block, modified to account for the additional $P$ factors,' and the $\tilde R$-sector contribution to the $0\mathrm{A}^-$ and $0\mathrm{B}^-$ torus amplitudes rests entirely on this postulate.

Editorial extensions

If this is right

  • If the amplitudes are correct, the super Virasoro minimal string duality of [25] is confirmed from the worldsheet, including the momentum-independent constant $-1/16$ amplitude of the $0\mathrm{A}^-$ theory with its hard-edge spectral curve.
  • The four string theories are cleanly distinguished by the GSO projection together with the relative sign of the total worldsheet supercharge, and the sign ambiguity in the timelike super Liouville structure constants is fixed by modular covariance.
  • The corrected torus blocks and the eight modular $S$-kernels are theory-independent $N=1$ kinematic data, so torus one-point functions of any $N=1$ SCFT can be assembled from them.
  • The exceptional zero-momentum Ramond insertion in $0\mathrm{A}^-$ is a worldsheet candidate for the Ramond punctures of JT supergravity and its dual matrix integral.

Reading between the lines

Editorial extensions of the paper, not claims the author makes directly.

  • The block decomposition of the distinguished superdescendant is theory-independent, so $\tilde R$-sector torus one-point functions of this operator in other $N=1$ SCFTs should follow by substituting their structure constants and spectral densities; the paper suggests this route but does not carry it out.
  • Summing a gas of the $0\mathrm{A}^-$ Ramond punctures should deform the hard-edge spectral curve of the dual matrix integral, in parallel with turning on Ramond-Ramond flux in the $\hat c=1$ Type 0A string; that sum is left as future work.
  • The kernel bootstrap strategy, fixed by analytic structure, parity, and idempotency rather than by solving Moore-Seiberg relations, should extend to $N=1$ fusion kernels for sphere four-point amplitudes and connect to the $U_q(\mathrm{osp}(1|2))$ 6j-symbols; the paper notes that this map is not yet precise.
Original abstract

Motivated by applications to low-dimensional worldsheet string constructions, we analyze $\mathcal{N} = 1$ super Liouville theory on the torus. Specifically, we re-examine the recursive representations of the torus one-point super Virasoro blocks that have been constructed in the literature and correct several of their ingredients. In the process we identify a new block in the odd spin structure, associated with a privileged superdescendant whose torus one-point function transforms like that of a Virasoro primary. We then demonstrate that the structure constants for both spacelike and timelike super Liouville theory satisfy modular crossing. Furthermore, we use a bootstrap argument to construct modular crossing kernels for all four spin structure sectors, valid for central charges $c \in \mathbb{C}\setminus(-\infty,\tfrac{3}{2}]$, and verify that they correctly implement the crossing transformations of the blocks. As a concrete application of the technology, we analyze the super Virasoro minimal string. There are four such theories, $\mathrm{0A}^{\pm}$ and $\mathrm{0B}^{\pm}$, which are distinguished by the GSO projection together with the choice of worldsheet supercharge. The resulting NS-sector sphere three-point and torus one-point amplitudes are shown to agree with topological recursion on the spectral curves of the dual matrix integrals, which were recently derived from 3d supergravity. Notably, the one-point function of the privileged superdescendant plays an essential role in the contribution of the odd spin structure to the torus amplitude via a careful treatment of the picture changing operator. We also identify an exceptional zero-momentum Ramond insertion in the $\mathrm{0A}^{-}$ theory that we interpret geometrically as a Ramond puncture, and match its mixed sphere three-point amplitude to the corresponding intersection theory prediction.

The compiled record

The paper's own sentences, arranged, kept beside the review and separate from it. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.

Compiled by classifier-1.13.0 via TypeSafe API, question bank abstract-p1-20260923, 2026-10-02: 1 request, 7,891 input tokens.

What the abstract itself states, as probabilities: claims first 0.04 · states limitation 0.19 · human participants 0.01 · controlled comparison 0.03 · randomized assignment 0.01 · states quantitative result 0.54 · compares with prior results 0.91 · mentions code or data availability 0.02.

The abstract, sentence by sentence

arXiv listing abstract v1. Results and the main claim are underlined; .

Motivated by applications to low-dimensional worldsheet string constructions, we analyze $\mathcal{N} = 1$ super Liouville theory on the torus. Specifically, we re-examine the recursive representations of the torus one-point super Virasoro blocks that have been constructed in the literature and correct several of their ingredients. In the process we identify a new block in the odd spin structure, associated with a privileged superdescendant whose torus one-point function transforms like that of a Virasoro primary. We then demonstrate that the structure constants for both spacelike and timelike super Liouville theory satisfy modular crossing. Furthermore, we use a bootstrap argument to construct modular crossing kernels for all four spin structure sectors, valid for central charges $c \in \mathbb{C}\setminus(-\infty,\tfrac{3}{2}]$, and verify that they correctly implement the crossing transformations of the blocks. As a concrete application of the technology, we analyze the super Virasoro minimal string. There are four such theories, $\mathrm{0A}^{\pm}$ and $\mathrm{0B}^{\pm}$, which are distinguished by the GSO projection together with the choice of worldsheet supercharge. The resulting NS-sector sphere three-point and torus one-point amplitudes are shown to agree with topological recursion on the spectral curves of the dual matrix integrals, which were recently derived from 3d supergravity. Notably, the one-point function of the privileged superdescendant plays an essential role in the contribution of the odd spin structure to the torus amplitude via a careful treatment of the picture changing operator. We also identify an exceptional zero-momentum Ramond insertion in the $\mathrm{0A}^{-}$ theory that we interpret geometrically as a Ramond puncture, and match its mixed sphere three-point amplitude to the corresponding intersection theory prediction.

background contribution method result interpretation main claim

What the classifier reports for each sentence. The number is the probability it gave the label.
#sentencerolethe authors' own workstates the main conclusionstrength
s0 Motivated by applications to low-dimensional worldsheet string constructions, we analyze $\mathcal{N} = 1$ super Liouville theory on the torus. contribution 0.69 0.69 0.04 asserted 0.87
s1 Specifically, we re-examine the recursive representations of the torus one-point super Virasoro blocks that have been constructed in the literature and correct several of their ingredients. contribution 0.89 0.86 0.05 asserted 0.99
s2 In the process we identify a new block in the odd spin structure, associated with a privileged superdescendant whose torus one-point function transforms like that of a Virasoro primary. result 0.89 0.95 0.13 asserted 1.00
s3 We then demonstrate that the structure constants for both spacelike and timelike super Liouville theory satisfy modular crossing. result 0.97 0.93 0.20 asserted 1.00
s4 Furthermore, we use a bootstrap argument to construct modular crossing kernels for all four spin structure sectors, valid for central charges $c \in \mathbb{C}\setminus(-\infty,\tfrac{3}{2}]$, and verify that they correctly implement the crossing transformations of the blocks. contribution 0.71 0.96 0.26 asserted 1.00
s5 As a concrete application of the technology, we analyze the super Virasoro minimal string. contribution 0.97 0.89 0.05 asserted 0.84
s6 There are four such theories, $\mathrm{0A}^{\pm}$ and $\mathrm{0B}^{\pm}$, which are distinguished by the GSO projection together with the choice of worldsheet supercharge. background 0.63 0.17 0.04 asserted 1.00
s7 The resulting NS-sector sphere three-point and torus one-point amplitudes are shown to agree with topological recursion on the spectral curves of the dual matrix integrals, which were recently derived from 3d supergravity. result 1.00 0.85 0.14 asserted 1.00
s8 Notably, the one-point function of the privileged superdescendant plays an essential role in the contribution of the odd spin structure to the torus amplitude via a careful treatment of the picture changing operator. result 0.69 0.86 0.10 asserted 1.00
s9 We also identify an exceptional zero-momentum Ramond insertion in the $\mathrm{0A}^{-}$ theory that we interpret geometrically as a Ramond puncture, and match its mixed sphere three-point amplitude to the corresponding intersection theory prediction. result 0.69 0.94 0.07 asserted 0.99

What kind of paper the classifier reports this is: theoretical result 1.00 · evidence from proof or derivation 1.00.

What was examined, and what was not

sources read
  • arXiv listing abstract v1
not examined
  • full text
  • figures and tables
  • references and citing sentences
  • relations to other papers
levels run
  • P abstract
not run
  • S sections
  • T body sentences
  • C citations
  • R cross-paper relations

Every quoted sentence on this record is the authors'. Every label is from Pith's closed vocabulary, with the probability shown beside it. Every number in the measurements table is the authors', checked by code. Record as JSON

Figures
Figure 1. Checks of modular covariance of the eight torus one-point functions for the spacelike and timelike super Liouville theories for the parameters scanned over the sets in (3.55). Numerical check of modular covariance: To verify that the identities (3.49), (3.50), and (3.54) hold we implemented the recursion relation numerically. Our explicit checks were carried out for the following parameters: b ∈ {3 4 , 4 5 , 3 π } , Pext ∈ { 3 10 , 1 2 , e π } . (3.55) 23
Figure 2. Checks of the eight S crossing kernels listed in (4.2). We check that each of them satisfies the crossing transformation (4.4). The values of the central charge used in each case are indicated in the legend. The momenta were chosen to be P0 = 0.04 + 0.03 i and Ps = 0.3 + 0.02 i. The kernels were integrated against the blocks as a function of Pt. We have extracted data for the deviation defined in (4.31) for a range of values of Im(τ ). 5 Applications: the super Virasoro minimal string As a concrete application of our considerations, we will analyze the worldsheet theory of the super…
Figure 3. String amplitudes for 0A± and 0B± theories. We plot the raw amplitudes computed at discrete values of the external momenta and compare them against the intersection theory and matrix model predictions. The last step involves fixing an overall normalization, which we explain later in the text. 44
Figure 4. Plot of the deviation of string amplitude from the expected matrix model result. It is instructive to dissect the amplitude and ask how the building blocks from the worldsheet behave. The correct combinations to consider are the modular invariant spin structure pieces. For the even spin structure numerical data supports the following NNS 4 CT2  I + 3 + I + 4 + I + 2  = 4 hext − 1 32 , NNS 4 CT2  I − 3 + I − 4 + I − 2  = − 1 32 . (5.39) The odd spin structure combinations also simplify, and turn out to be related to the even spin structure result. Explicitly, I + 1 = 1 3  I + 3…

Figures reproduced from arXiv:2610.01909 by the authors.

References

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