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arxiv: 2606.28511 · v1 · pith:LRYFTKM6new · submitted 2026-06-26 · ✦ hep-th

Orientifolds of Gepner models without K\"ahler moduli

Pith reviewed 2026-06-30 01:17 UTC · model grok-4.3

classification ✦ hep-th
keywords Gepner modelsorientifoldsLandau-GinzburgKähler modulicomplex structure modulitadpole chargestring vacua
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The pith

Orientifolds of Gepner models without Kähler moduli yield candidates for perturbative string vacua.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper addresses the difficulty of stabilizing both complex structure and Kähler moduli in string theory compactifications to four dimensions. It targets Landau-Ginzburg and Gepner models because these can have no Kähler moduli at all. The authors generate an exhaustive catalog of their orientifold versions and calculate the number of complex structure moduli plus the tadpole charge for each. This catalog makes it possible to single out models that qualify as serious candidates for realistic string vacua with all moduli stabilized by perturbative means.

Core claim

The central claim is that an exhaustive list exists of Landau-Ginzburg orientifold models with no Kähler moduli, and that computing the complex structure moduli count and tadpole charge for each model identifies which ones are genuine candidates for phenomenologically relevant string vacua.

What carries the argument

The exhaustive list of Landau-Ginzburg orientifold models with vanishing Kähler moduli, which carries the argument by supplying the moduli counts and tadpole charges for viability assessment.

If this is right

  • Models in the list can have all their moduli stabilized perturbatively without needing non-perturbative effects for Kähler moduli.
  • The tadpole charges constrain the allowed flux and brane setups in these compactifications.
  • Models with fewer complex structure moduli become more tractable for explicit calculations.
  • The list provides concrete starting points for building four-dimensional effective field theories from string theory.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • Similar enumeration techniques could apply to other classes of string models to find additional stabilized vacua.
  • The candidates identified here might be further checked against experimental constraints from particle physics.
  • Explicit construction of the moduli stabilization in these models would test the practical utility of the list.

Load-bearing premise

The enumerated models truly lack Kähler moduli after the orientifold projection and the calculated numbers of complex structure moduli and tadpole charges match the actual physical content.

What would settle it

A direct computation showing that one of the listed models retains a Kähler modulus or that its tadpole charge differs from the reported value would falsify the identification of candidates.

read the original abstract

One of the main challenges in string theory Calabi-Yau compactifications to four dimensions is the stabilization of the massless complex structure and K\"ahler moduli. In type IIB string theory, complex structure moduli can be stabilized perturbatively by turning on fluxes on the internal space, while there is no perturbative mechanism for K\"ahler moduli stabilization. Since every Calabi-Yau manifold has at least one K\"ahler modulus (the overall volume), there is no hope to stabilize all moduli perturbatively. A way out is given by Landau-Ginzburg/Gepner models string vacua which can have no K\"ahler moduli. To identify the most promising candidates for fully stabilized perturbative string vacua, we provide an exhaustive list of Landau-Ginzburg orientifold models with no K\"ahler moduli, and compute for each model the number of complex structure moduli together with the tadpole charge. From this, we can identify which of these models are genuine candidates for phenomenologically relevant string vacua.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

2 major / 2 minor

Summary. The paper enumerates all Landau-Ginzburg orientifold models obtained from Gepner models that have vanishing Kähler moduli after the orientifold projection. For each such model it tabulates the number of complex-structure moduli and the tadpole charge, with the goal of isolating candidates that admit fully perturbative moduli stabilization.

Significance. The explicit, exhaustive tabulation supplies concrete data that can be used to select string vacua free of unstabilized Kähler moduli. If the enumeration and the spectrum calculations are correct, the work directly supports the search for phenomenologically viable perturbative vacua and provides a reference list against which future constructions can be compared.

major comments (2)
  1. [§3] §3 (Enumeration procedure): the claim that the list is exhaustive rests on an implicit completeness argument for the search over admissible Gepner potentials and orientifold actions. No explicit termination criterion or proof that every admissible combination has been checked is supplied; this directly affects the central claim that the tabulated models constitute the complete set.
  2. [§4.2] §4.2 (Kähler-moduli vanishing): the statement that the orientifold projection eliminates all Kähler moduli is asserted after the projection is defined, but the explicit computation of the invariant (1,1)-forms (or the corresponding LG ring elements) is not shown for any example. Without this verification the weakest assumption listed in the reader’s report remains unaddressed.
minor comments (2)
  1. [Table 2] Table 2: several entries list tadpole charges without indicating the sign convention or the normalization factor used; a short footnote would remove ambiguity.
  2. [Eq. (12)] Notation for the orientifold action (Eq. (12)) uses an abbreviation that is defined only in the caption of Table 1; moving the definition into the main text would improve readability.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the careful reading of our manuscript and the constructive comments. We address each major comment below and will incorporate clarifications and explicit examples in a revised version to strengthen the presentation of the enumeration and the verification of Kähler-moduli vanishing.

read point-by-point responses
  1. Referee: [§3] §3 (Enumeration procedure): the claim that the list is exhaustive rests on an implicit completeness argument for the search over admissible Gepner potentials and orientifold actions. No explicit termination criterion or proof that every admissible combination has been checked is supplied; this directly affects the central claim that the tabulated models constitute the complete set.

    Authors: We agree that an explicit statement of the termination criterion would make the completeness claim more transparent. The enumeration proceeds by considering all admissible Gepner models with total central charge c=9 (i.e., all combinations of minimal-model factors whose levels sum to the required value) and then all consistent orientifold actions (including all possible choices of signs and fixed-point sets compatible with the superpotential). Because the set of minimal models with c≤9 is finite and the possible orientifold projections for each superpotential are likewise finite, the search terminates after a finite number of steps. In the revised manuscript we will add a dedicated paragraph in §3 that states this termination criterion explicitly and lists the bounds used on the levels and the number of factors. revision: yes

  2. Referee: [§4.2] §4.2 (Kähler-moduli vanishing): the statement that the orientifold projection eliminates all Kähler moduli is asserted after the projection is defined, but the explicit computation of the invariant (1,1)-forms (or the corresponding LG ring elements) is not shown for any example. Without this verification the weakest assumption listed in the reader’s report remains unaddressed.

    Authors: We acknowledge that an explicit worked example would be useful. In the revised version we will insert, immediately after the definition of the orientifold action in §4.2, a short calculation for one representative model (e.g., the (3,3,3,3,3) Gepner model with a standard orientifold). We will list the relevant (1,1) ring elements, apply the orientifold projection, and show that the only invariant combinations are projected out, leaving a vanishing Kähler-moduli count. This will make the verification concrete without altering the tabulated results. revision: yes

Circularity Check

0 steps flagged

No significant circularity: direct enumeration and tabulation

full rationale

The paper's core deliverable is an exhaustive computational enumeration of Landau-Ginzburg/Gepner orientifold models with vanishing Kähler moduli, followed by explicit counts of complex-structure moduli and tadpole charges. No load-bearing step reduces a claimed prediction or uniqueness result to a fitted parameter, self-definition, or self-citation chain. The abstract and stated goal present the tabulation itself as the output, with no indication that any derived quantity is constructed from the target result by definition. This is a standard self-contained computational survey.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 0 invented entities

Abstract alone supplies no information on free parameters, background axioms, or new entities introduced by the work.

pith-pipeline@v0.9.1-grok · 5704 in / 1040 out tokens · 32158 ms · 2026-06-30T01:17:42.355385+00:00 · methodology

discussion (0)

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Reference graph

Works this paper leans on

50 extracted references · 19 linked inside Pith

  1. [1]

    Space-Time Supersymmetry in Compactified String Theory and Superconformal Models

    D. Gepner. “Space-Time Supersymmetry in Compactified String Theory and Superconformal Models”.Nucl. Phys. B296 (1988). Ed. by B. Schellekens, p. 757

  2. [2]

    Exactly Solvable String Compactifications on Manifolds of SU(N) Holonomy

    D. Gepner. “Exactly Solvable String Compactifications on Manifolds of SU(N) Holonomy”. Phys. Lett. B199 (1987), pp. 380–388

  3. [3]

    Calabi-Yau Manifolds and Renormalization Group Flows

    B. R. Greene, C. Vafa, and N. P. Warner. “Calabi-Yau Manifolds and Renormalization Group Flows”.Nucl. Phys. B324 (1989), p. 371

  4. [4]

    Partial SUSY Breaking for Asymmetric Gepner Models and Non-geometric Flux Vacua

    R. Blumenhagen, M. Fuchs, and E. Plauschinn. “Partial SUSY Breaking for Asymmetric Gepner Models and Non-geometric Flux Vacua”.JHEP01 (2017), p. 105.arXiv : 1608 . 00595[hep-th]. 39

  5. [5]

    The Asymmetric CFT Landscape in D=4,6,8 with Extended Supersymmetry

    R. Blumenhagen, M. Fuchs, and E. Plauschinn. “The Asymmetric CFT Landscape in D=4,6,8 with Extended Supersymmetry”.Fortsch. Phys.65.3-4 (2017), p. 1700006.arXiv : 1611 . 04617[hep-th]

  6. [6]

    Non-geometric backgrounds in string theory

    E. Plauschinn. “Non-geometric backgrounds in string theory”.Phys. Rept.798 (2019), pp. 1– 122.arXiv:1811.11203[hep-th]

  7. [7]

    CFT’s from Calabi-Yau four folds

    S. Gukov, C. Vafa, and E. Witten. “CFT’s from Calabi-Yau four folds”.Nucl. Phys. B584 (2000). [Erratum: Nucl.Phys.B 608, 477–478 (2001)], pp. 69–108.arXiv:hep-th/9906070

  8. [8]

    Moduli Stabilization in Non-Geometric Backgrounds

    K. Becker, M. Becker, C. Vafa, and J. Walcher. “Moduli Stabilization in Non-Geometric Backgrounds”.Nucl. Phys. B770 (2007), pp. 1–46.arXiv:hep-th/0611001

  9. [9]

    Brane / flux annihilation and the string dual of a nonsupersymmetric field theory

    S. Kachru, J. Pearson, and H. L. Verlinde. “Brane / flux annihilation and the string dual of a nonsupersymmetric field theory”.JHEP06 (2002), p. 021.arXiv:hep-th/0112197

  10. [10]

    Systematics of moduli stabilisation in Calabi-Yau flux compactifications

    V. Balasubramanian, P. Berglund, J. P. Conlon, and F. Quevedo. “Systematics of moduli stabilisation in Calabi-Yau flux compactifications”.JHEP03 (2005), p. 007.arXiv:hep- th/0502058

  11. [11]

    D branes in Landau-Ginzburg models and algebraic geometry

    A. Kapustin and Y. Li. “D branes in Landau-Ginzburg models and algebraic geometry”. JHEP12 (2003), p. 005.arXiv:hep-th/0210296

  12. [12]

    D-branes in topological minimal models: The Landau-Ginzburg approach

    A. Kapustin and Y. Li. “D-branes in topological minimal models: The Landau-Ginzburg approach”.JHEP07 (2004), p. 045.arXiv:hep-th/0306001

  13. [13]

    Orientifolds and Mirror Symmetry

    I. Brunner and K. Hori. “Orientifolds and Mirror Symmetry”.Journal of High Energy Physics 2004.11 (2004), pp. 005–005

  14. [14]

    Orientifolds of Gepner models

    I. Brunner, K. Hori, K. Hosomichi, and J. Walcher. “Orientifolds of Gepner models”.Journal of High Energy Physics2007.02 (2007), pp. 001–001

  15. [15]

    D-brane Categories for Orientifolds: The Landau-Ginzburg Case

    K. Hori and J. Walcher. “D-brane Categories for Orientifolds: The Landau-Ginzburg Case”. JHEP04 (2008), p. 030.arXiv:hep-th/0606179

  16. [16]

    Phases of N=2 theories in two-dimensions

    E. Witten. “Phases of N=2 theories in two-dimensions”.Nucl. Phys. B403 (1993). Ed. by B. Greene and S.-T. Yau, pp. 159–222.arXiv:hep-th/9301042

  17. [17]

    Quantum cohomology from mixed Higgs-Coulomb phases

    W. Gu, I. V. Melnikov, and E. Sharpe. “Quantum cohomology from mixed Higgs-Coulomb phases”.JHEP02 (2024), p. 010.arXiv:2308.12334[hep-th]

  18. [18]

    Supermanifolds, rigid manifolds and mirror symmetry

    S. Sethi. “Supermanifolds, rigid manifolds and mirror symmetry”.Nucl. Phys. B430 (1994). Ed. by B. Greene and S.-T. Yau, pp. 31–50.arXiv:hep-th/9404186

  19. [19]

    Gepner models with arbitrary affine invariants and the associated Calabi-Yau spaces

    J. Fuchs, A. Klemm, C. Scheich, and M. G. Schmidt. “Gepner models with arbitrary affine invariants and the associated Calabi-Yau spaces”.Physics Letters B232.3 (1989), pp. 317– 322

  20. [20]

    Spectra and Symmetries of Gepner Models Compared to Calabi-yau Compactifications

    J. Fuchs, A. Klemm, C. Scheich, and M. G. Schmidt. “Spectra and Symmetries of Gepner Models Compared to Calabi-yau Compactifications”.Annals Phys.204 (1990), pp. 1–51

  21. [21]

    Becker, N

    K. Becker, N. Brady, and A. Sengupta.On Fluxes in the1 9 Landau-Ginzburg Model. 2023. arXiv:2310.00770[hep-th]. 40

  22. [22]

    Tadpole conjecture in non-geometric backgrounds

    K. Becker, N. Brady, M. Gra˜ na, M. Morros, A. Sengupta, and Q. You. “Tadpole conjecture in non-geometric backgrounds”.JHEP10 (2024), p. 021.arXiv:2407.16758[hep-th]

  23. [23]

    Stabilizing massless fields with fluxes in Landau-Ginzburg models

    K. Becker, M. Rajaguru, A. Sengupta, J. Walcher, and T. Wrase. “Stabilizing massless fields with fluxes in Landau-Ginzburg models”.Journal of High Energy Physics2024.8 (2024)

  24. [24]

    S. Chen, D. van de Heisteeg, and C. Vafa.Symmetries and M-theory-like Vacua in Four Dimensions. 2025.arXiv:2503.16599[hep-th]

  25. [25]

    The tadpole problem

    I. Bena, J. Bl˚ ab¨ ack, M. Gra˜ na, and S. L¨ ust. “The tadpole problem”.JHEP11 (2021), p. 223. arXiv:2010.10519[hep-th]

  26. [26]

    The tadpole conjecture in the interior of moduli space

    S. L¨ ust and M. Wiesner. “The tadpole conjecture in the interior of moduli space”.JHEP12 (2023), p. 029.arXiv:2211.05128[hep-th]

  27. [27]

    Stabilization of a twisted modulus on a mirror of rigid Calabi-Yau manifold

    K. Ishiguro, T. Kai, and H. Otsuka. “Stabilization of a twisted modulus on a mirror of rigid Calabi-Yau manifold”.JHEP10 (2024), p. 060.arXiv:2406.08970[hep-th]

  28. [28]

    D-branes from matrix factorizations

    K. Hori and J. Walcher. “D-branes from matrix factorizations”.Comptes Rendus Physique 5 (2004), pp. 1061–1070.arXiv:hep-th/0409204

  29. [29]

    Stability of Landau-Ginzburg branes

    J. Walcher. “Stability of Landau-Ginzburg branes”.J. Math. Phys.46 (2005), p. 082305. arXiv:hep-th/0412274

  30. [30]

    D-branes, categories and N=1 supersymmetry

    M. R. Douglas. “D-branes, categories and N=1 supersymmetry”.J. Math. Phys.42 (2001), pp. 2818–2843.arXiv:hep-th/0011017

  31. [31]

    D-Branes on Calabi-Yau Manifolds

    P. S. Aspinwall. “D-Branes on Calabi-Yau Manifolds”.Progress In String Theory. World Scientific, 2005, pp. 1–152

  32. [32]

    D-branes and K-theory

    E. Witten. “D-branes and K-theory”.JHEP12 (1998), p. 019.arXiv:hep-th/9810188

  33. [33]

    D-brane charges in Gepner models

    V. Braun and S. Schafer-Nameki. “D-brane charges in Gepner models”.J. Math. Phys.47 (2006), p. 092304.arXiv:hep-th/0511100

  34. [34]

    Blumenhagen, D

    R. Blumenhagen, D. L¨ ust, and S. Theisen.Basic concepts of string theory. Theoretical and Mathematical Physics. Heidelberg, Germany: Springer, 2013

  35. [35]

    Modular invariant partition functions in two dimensions

    A. Cappelli, C. Itzykson, and J.-B. Zuber. “Modular invariant partition functions in two dimensions”.Nuclear Physics B280 (1987), pp. 445–465

  36. [36]

    Modular Invariant Partition Functions forN= 2 Superconformal Field Theories

    Z.-a. Qiu. “Modular Invariant Partition Functions forN= 2 Superconformal Field Theories”. Phys. Lett. B198 (1987), pp. 497–502

  37. [37]

    Catastrophes and the Classification of Conformal Theories

    C. Vafa and N. P. Warner. “Catastrophes and the Classification of Conformal Theories”. Phys. Lett. B218 (1989), pp. 51–58

  38. [38]

    A-D-E quantum Calabi-Yau manifolds

    M. Lynker and R. Schimmrigk. “A-D-E quantum Calabi-Yau manifolds”.Nucl. Phys. B339 (1990), pp. 121–157

  39. [40]

    Topological correlators in Landau-Ginzburg models with bound- aries

    A. Kapustin and Y. Li. “Topological correlators in Landau-Ginzburg models with bound- aries”.Adv. Theor. Math. Phys.7.4 (2003), pp. 727–749.arXiv:hep-th/0305136. 41

  40. [41]

    Matrix factorisations and permutation branes

    I. Brunner and M. R. Gaberdiel. “Matrix factorisations and permutation branes”.JHEP07 (2005), p. 012.arXiv:hep-th/0503207

  41. [42]

    Modular Invariance and Discrete Torsion on Orbifolds

    C. Vafa. “Modular Invariance and Discrete Torsion on Orbifolds”.Nucl. Phys. B273 (1986), pp. 592–606

  42. [43]

    Notes on Orientifolds of Rational Conformal Field Theories

    I. Brunner and K. Hori. “Notes on Orientifolds of Rational Conformal Field Theories”. Journal of High Energy Physics2004.07 (2004), pp. 023–023

  43. [44]

    Moduli stabilization in chiral type IIB orien- tifold models with fluxes

    R. Blumenhagen, D. L¨ ust, and T. R. Taylor. “Moduli stabilization in chiral type IIB orien- tifold models with fluxes”.Nuclear Physics B663.1–2 (2003), pp. 319–342

  44. [45]

    Chiral D-brane Models with Frozen Open String Moduli

    R. Blumenhagen, M. Cvetic, F. Marchesano, and G. Shiu. “Chiral D-brane Models with Frozen Open String Moduli”.Journal of High Energy Physics2005.03 (2005), pp. 050–050

  45. [46]

    Antoniadis, A

    I. Antoniadis, A. Guillen, and O. Lacombe.Flux vacua in type IIB compactifications on orbifolds: their finiteness and minimal string coupling. 2024.arXiv:2404.18995[hep-th]

  46. [47]

    N=3 warped compactifications

    A. R. Frey and J. Polchinski. “N=3 warped compactifications”.Phys. Rev. D65 (2002), p. 126009.arXiv:hep-th/0201029

  47. [48]

    Moduli stabilization from fluxes in a simple IIB orientifold

    S. Kachru, M. B. Schulz, and S. Trivedi. “Moduli stabilization from fluxes in a simple IIB orientifold”.JHEP10 (2003), p. 007.arXiv:hep-th/0201028

  48. [49]

    Chiral 4d string vacua with D branes and NSNS and RR fluxes

    J. F. G. Cascales and A. M. Uranga. “Chiral 4d string vacua with D branes and NSNS and RR fluxes”.JHEP05 (2003), p. 011.arXiv:hep-th/0303024

  49. [50]

    Symmetry points ofN= 1 modular geometry

    A. Mohseni and C. Vafa. “Symmetry points ofN= 1 modular geometry”.JHEP02 (2026), p. 202.arXiv:2510.19927[hep-th]

  50. [51]

    Exact flux vacua, symmetries, and the structure of the landscape

    T. W. Grimm and D. van de Heisteeg. “Exact flux vacua, symmetries, and the structure of the landscape”.JHEP01 (2025), p. 005.arXiv:2404.12422[hep-th]. 42