pith. machine review for the scientific record. sign in

arxiv: 2603.12315 · v2 · submitted 2026-03-12 · ✦ hep-th

Recognition: 2 theorem links

· Lean Theorem

Quantum obstructions for N=1 infinite distance limits -- Part I: g_s obstructions

Authors on Pith no claims yet

Pith reviewed 2026-05-15 11:34 UTC · model grok-4.3

classification ✦ hep-th
keywords infinite distance limitsType IIB orientifoldsg_s correctionsF-theorymoduli spaceO7-planesCalabi-Yau fourfoldsquantum obstructions
0
0 comments X

The pith

Non-perturbative g_s corrections in Type IIB orientifolds can become unsuppressed in infinite distance limits and lift classical degenerations.

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

The paper studies quantum effects that block classical infinite distance limits in the complex structure moduli space of four-dimensional N=1 Type IIB orientifolds with O7- and O3-planes. These limits appear in asymptotic regions of field space that are used for model building and cosmology. By lifting the setup to F-theory, the authors encode all pure g_s corrections inside the classical geometry of an elliptic Calabi-Yau fourfold. They find that the resulting quantum-corrected moduli space deviates from the classical one, with non-perturbative g_s effects growing large when the O7-plane sits at certain positions. In extreme cases the entire classical degeneration is removed.

Core claim

The g_s-corrected moduli space obtained from the elliptic Calabi-Yau fourfold differs from the classical Type IIB moduli space. Non-perturbative corrections in the string coupling become unsuppressed in large complex structure limits and other infinite distance regions, obstructing a perturbative Type IIB description. Depending on the location of the O7-plane, these corrections can completely eliminate the classical infinite distance degeneration at the quantum level.

What carries the argument

The classical geometry of the elliptic Calabi-Yau fourfold that encodes all pure g_s corrections and yields the quantum-corrected moduli space of the Type IIB orientifold.

If this is right

  • A perturbative Type IIB effective action ceases to be valid in certain asymptotic regions of the moduli space.
  • Some classical infinite distance limits do not survive once g_s corrections are included.
  • The position of the O7-plane determines whether the corrections remain under control.
  • The quantum-corrected moduli space must be used instead of the classical one for reliable string model building near these limits.

Where Pith is reading between the lines

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

  • Quantum corrections may need to be incorporated into statements of the distance conjecture in N=1 settings.
  • Model-building scenarios that rely on classical infinite distance limits for large field ranges require re-examination once g_s effects are accounted for.
  • The same F-theory encoding could be applied to test whether alpha-prime corrections produce similar obstructions in the companion analysis.

Load-bearing premise

All pure g_s corrections are captured by the classical geometry of the elliptic Calabi-Yau fourfold, and the O7-plane location alone decides whether those corrections stay suppressed.

What would settle it

A concrete Calabi-Yau orientifold example in which a classical large complex structure limit remains an infinite distance point after the full g_s-corrected metric is computed from the elliptic fourfold.

Figures

Figures reproduced from arXiv: 2603.12315 by Jeroen Monnee, Lukas Kaufmann, Max Wiesner, Timo Weigand.

Figure 1
Figure 1. Figure 1: A semi-stable degeneration as in (3.10) in which the central fiber V0 splits into the union of two components V1 and V2 that intersect over V12. and their union as V (k+1) = G i0,...,ik Vi0···ik , 0 ≤ k ≤ 3 . (3.13) These spaces are conveniently combined into the so-called dual (intersection) graph Π(V0) of V0. The latter is a simplicial complex that is defined inductively as follows. First, to each compon… view at source ↗
Figure 2
Figure 2. Figure 2: An example of an O-type A/B orientifold in a two-component type II degeneration, in which the threefold splits into two components V1 and V2, intersecting over the double surface V12. In the O-type A limit, the O7-plane (indicated in red) wraps the whole double surface V12, whereas in the O-type B limit it intersects it in codimension 1. Geometric details on this Calabi–Yau threefold can be found in Append… view at source ↗
Figure 3
Figure 3. Figure 3: The dual graphs (a) Π(V ϕ1 0 ) and (b) Π(V ϕ2 0 ) corresponding to the type III limit ϕ1 → ∞ and the type II limit ϕ2 → ∞, respectively. The action of the two O-type A orientifolds and the resulting orientifolded dual graph are depicted in blue. In both cases the orientifold action reduces the dimension of the dual graph by one. The action of the orientifold on the dual graph exchanges two vertices of the … view at source ↗
Figure 4
Figure 4. Figure 4: (a) For O-type A limits, the divisors ∆S and ∆F intersect in a point of tangency from the Type IIB perspective. (b) In the F-theory moduli space, the point of tangency can be resolved via blow-up, introducing an exceptional divisor ∆ˆ F S. concrete choice of Weierstrass model, does not have to. This is a further indication that the modulus responsible for the degeneration (4.6) encodes open-string informat… view at source ↗
Figure 5
Figure 5. Figure 5: Behaviour along ∆ˆ F . We begin with the limit ϕ˜ 2 → ∞ in the F-theory moduli space with all other moduli at generic values and, in particular, away from weak coupling. To this end, we parametrise the base hypersurface as B3,ϕ˜ 2 = {ϕ˜ 2(k − p 2 ) 2 + Q12 = 0} ⊂ P 4 2,2,2,3,6 /GGP , Q12 generic . (4.13) Notice that (k − p 2 ) 2 is indeed invariant under Gσ GP. The limit ϕ˜ 2 → ∞ amounts to imposing the ba… view at source ↗
Figure 5
Figure 5. Figure 5: An illustration of the quantum moduli space for the F-theory lift of the type II O-type A limit ϕ2 → ∞ in the mirror of P 4 2,2,2,3,3 [12]. (a) A generic point on ∆ˆ S, where the fourfold W undergoes the standard Sen-limit. (b) A generic point on ∆ˆ F , where the base becomes B3,0 = {(p 2 − h) 2 = 0}/GGP, which is smooth. For generic g, W is smooth, but can acquire Kodaira type III singularities in codimen… view at source ↗
Figure 6
Figure 6. Figure 6: A sketch of the discriminant locus in the complex structure moduli space of the mirror of P 4 1,1,1,6,9 [18]. Reproduced from [PITH_FULL_IMAGE:figures/full_fig_p034_6.png] view at source ↗
read the original abstract

We analyse quantum obstructions to classical infinite distance limits in four-dimensional string compactifications with N=1 supersymmetry. Such quantum effects signal a severe departure from the perturbative effective action and can be of considerable importance for string model building. Our focus is on the complex structure moduli space of Type IIB orientifolds with O7/O3-planes and its F-theory description. In this first part of our analysis, we investigate the behaviour of $g_s$ corrections in infinite distance complex structure limits. Our main finding is that, depending on the location of the O7-plane, non-perturbative corrections in $g_s$ can become unsuppressed, thus obstructing a perturbative Type IIB description in the corresponding asymptotic region of the field space. In particular, this applies to large complex structure limits. To show this, we study the F-theory description of the Type IIB orientifold, in which all pure $g_s$ corrections are encoded in the (classical) geometry of an elliptic Calabi-Yau fourfold. This $g_s$-corrected moduli space is found to differ significantly from the classical moduli space. In extreme cases the classical infinite distance degeneration can be completely removed at the $g_s$-corrected quantum level. The behaviour of $\alpha'$ corrections, as well as implications for string model building, are discussed in a companion paper.

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

1 major / 1 minor

Summary. The manuscript analyzes quantum obstructions to classical infinite distance limits in N=1 four-dimensional string compactifications, focusing on g_s corrections in the complex structure moduli space of Type IIB orientifolds with O7/O3-planes. Using the F-theory description on an elliptic Calabi-Yau fourfold, it claims that non-perturbative g_s corrections can become unsuppressed depending on O7-plane location, obstructing a perturbative Type IIB description in asymptotic regions and, in extreme cases, removing the classical degeneration entirely.

Significance. If the central claim holds, the work would be significant for the swampland program and string model building, as it provides a geometric mechanism by which quantum g_s effects qualitatively alter the structure of infinite-distance limits in N=1 moduli spaces. The encoding of all pure g_s corrections via the classical elliptic fourfold geometry offers a concrete tool for identifying when perturbative descriptions break down.

major comments (1)
  1. [F-theory description section] F-theory description section: The load-bearing assumption that every pure g_s correction (including non-perturbative terms that become unsuppressed) is exactly captured by the classical geometry of the elliptic Calabi-Yau fourfold obtained from the Type IIB orientifold lift is asserted but not shown to be exhaustive for infinite-distance complex-structure limits; the mapping from O7/D7 data to the Weierstrass model may miss localized worldsheet or D-instanton contributions outside the fourfold geometry.
minor comments (1)
  1. [Abstract] Abstract: The distinction between the classical Type IIB moduli space and the g_s-corrected F-theory moduli space could be stated more explicitly to clarify the scope of the obstruction result.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for their careful reading of the manuscript and for the constructive feedback. We address the single major comment below and will incorporate clarifications in the revised version.

read point-by-point responses
  1. Referee: [F-theory description section] F-theory description section: The load-bearing assumption that every pure g_s correction (including non-perturbative terms that become unsuppressed) is exactly captured by the classical geometry of the elliptic Calabi-Yau fourfold obtained from the Type IIB orientifold lift is asserted but not shown to be exhaustive for infinite-distance complex-structure limits; the mapping from O7/D7 data to the Weierstrass model may miss localized worldsheet or D-instanton contributions outside the fourfold geometry.

    Authors: We agree that the manuscript would benefit from a more explicit justification of this point, particularly for the asymptotic regimes under consideration. The F-theory lift encodes all pure g_s corrections through the elliptic fibration and Weierstrass model because the axio-dilaton profile and 7-brane backreaction are fully determined by the geometry; this is a standard result in the literature on F-theory orientifold limits. Nevertheless, we acknowledge that the current text asserts rather than derives the exhaustiveness specifically for infinite-distance complex-structure limits. We will revise the F-theory description section to add a concise explanatory paragraph, supported by references, showing why no additional localized worldsheet or D-instanton effects arise outside the fourfold geometry for the pure g_s sector of the moduli effective action. This addresses the concern without altering the central claims. revision: yes

Circularity Check

0 steps flagged

No circularity: derivation uses standard F-theory encoding as external input

full rationale

The paper's central result—that non-perturbative g_s corrections can become unsuppressed depending on O7-plane location—follows from analyzing the moduli space geometry of the elliptic Calabi-Yau fourfold in the F-theory lift. The statement that 'all pure g_s corrections are encoded in the (classical) geometry of an elliptic Calabi-Yau fourfold' is invoked as an established correspondence rather than derived or fitted inside the paper's own equations. No step equates a 'prediction' to a fitted parameter by construction, renames a known result, or reduces the obstruction claim to a self-citation chain whose content is unverified within this work. The analysis of large-complex-structure limits and degeneration removal is therefore self-contained against the geometric input.

Axiom & Free-Parameter Ledger

0 free parameters · 2 axioms · 0 invented entities

The analysis rests on standard domain assumptions of string theory and F-theory rather than new free parameters or invented entities.

axioms (2)
  • domain assumption N=1 supersymmetry in four-dimensional string compactifications
    Stated as the setting for the orientifold models under study.
  • domain assumption All pure g_s corrections are encoded in the classical geometry of an elliptic Calabi-Yau fourfold
    Central encoding step that allows the quantum analysis to be performed geometrically.

pith-pipeline@v0.9.0 · 5553 in / 1240 out tokens · 29147 ms · 2026-05-15T11:34:00.255268+00:00 · methodology

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Lean theorems connected to this paper

Citations machine-checked in the Pith Canon. Every link opens the source theorem in the public Lean library.

What do these tags mean?
matches
The paper's claim is directly supported by a theorem in the formal canon.
supports
The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
extends
The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
uses
The paper appears to rely on the theorem as machinery.
contradicts
The paper's claim conflicts with a theorem or certificate in the canon.
unclear
Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.

Forward citations

Cited by 3 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score.

  1. On Quantum Obstructions in Type IIA Orientifolds

    hep-th 2026-04 unverdicted novelty 6.0

    Quantum corrections obstruct infinite distance limits in Type IIA orientifold Kähler moduli unless other moduli are also taken to infinity, as shown by worldsheet EFT strings, massless towers, and M-theory G2 uplifts.

  2. Towards the Realization of the Dark Dimension Scenario in Ho\v{r}ava-Witten Theory

    hep-th 2026-05 unverdicted novelty 5.0

    Hořava-Witten theory offers a potential string embedding of the dark dimension by localizing the Standard Model on the 11th interval, with symmetric tadpole cancellation and an infinite-distance limit helping derive t...

  3. Dark energy from string theory: an introductory review

    hep-th 2026-03 unverdicted novelty 2.0

    String theory imposes constraints on dark energy but permits various construction attempts for de Sitter vacua and single-field exponential quintessence models despite obstructions.

Reference graph

Works this paper leans on

103 extracted references · 103 canonical work pages · cited by 3 Pith papers · 53 internal anchors

  1. [1]

    Dine and N

    M. Dine and N. Seiberg,Is the Superstring Weakly Coupled?,Phys. Lett. B162(1985) 299

  2. [2]

    de Sitter Vacua in String Theory

    S. Kachru, R. Kallosh, A. D. Linde and S. P. Trivedi,De Sitter vacua in string theory, Phys. Rev. D68(2003) 046005 [hep-th/0301240]

  3. [3]

    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) 007 [hep-th/0502058]

  4. [4]

    J. P. Conlon, F. Quevedo and K. Suruliz,Large-volume flux compactifications: Moduli spectrum and D3/D7 soft supersymmetry breaking,JHEP08(2005) 007 [hep-th/0505076]

  5. [5]

    Kaufmann, J

    L. Kaufmann, J. Monnee, T. Weigand and M. Wiesner,Quantum obstructions for N= 1infinite distance limits – Part II: K¨ ahler obstructions,2603.13470

  6. [6]

    T. W. Grimm, E. Palti and I. Valenzuela,Infinite Distances in Field Space and Massless Towers of States,JHEP08(2018) 143 [1802.08264]

  7. [7]

    T. W. Grimm, C. Li and E. Palti,Infinite Distance Networks in Field Space and Charge Orbits,JHEP03(2019) 016 [1811.02571]. 43

  8. [8]

    Joshi and A

    A. Joshi and A. Klemm,Swampland Distance Conjecture for One-Parameter Calabi-Yau Threefolds,JHEP08(2019) 086 [1903.00596]

  9. [9]

    Bastian, T

    B. Bastian, T. W. Grimm and D. van de Heisteeg,Weak gravity bounds in asymptotic string compactifications,JHEP06(2021) 162 [2011.08854]

  10. [10]

    Gendler and I

    N. Gendler and I. Valenzuela,Merging the weak gravity and distance conjectures using BPS extremal black holes,JHEP01(2021) 176 [2004.10768]

  11. [11]

    Palti,Stability of BPS states and weak coupling limits,JHEP08(2021) 091 [2107.01539]

    E. Palti,Stability of BPS states and weak coupling limits,JHEP08(2021) 091 [2107.01539]

  12. [12]

    T. W. Grimm, S. Lanza and C. Li,Tameness, Strings, and the Distance Conjecture, JHEP09(2022) 149 [2206.00697]

  13. [13]

    T. W. Grimm, S. Lanza and T. van Vuren,Global symmetry-breaking and generalized theta-terms in Type IIB EFTs,JHEP10(2023) 154 [2211.11769]

  14. [14]

    Hassfeld, J

    B. Hassfeld, J. Monnee, T. Weigand and M. Wiesner,Emergent strings in Type IIB Calabi-Yau compactifications,JHEP01(2026) 140 [2504.01066]

  15. [15]

    Monnee, T

    J. Monnee, T. Weigand and M. Wiesner,Physics and geometry of complex structure limits in type IIB Calabi-Yau compactifications,JHEP03(2026) 063 [2509.07056]

  16. [16]

    Monnee, T

    J. Monnee, T. Weigand and M. Wiesner,K points and type IIB/heterotic duality with NS5-branes,Phys. Rev. D113(2026) 066002 [2510.02435]

  17. [17]

    Hattab, E

    J. Hattab, E. Palti and J. Quirant,On the K-point in moduli space,2509.11949

  18. [18]

    Hattab and E

    J. Hattab and E. Palti,On Type II 0 Loci in Moduli Space,2603.07746

  19. [19]

    Schmid,Variation of Hodge structure: the singularities of the period mapping, Invent

    W. Schmid,Variation of Hodge structure: the singularities of the period mapping, Invent. Math. , 22:211–319, 1973(1973)

  20. [20]

    Cattani, A

    E. Cattani, A. Kaplan and W. Schmid,Degeneration of Hodge Structures,Annals of Mathematics123(1986) 457

  21. [21]

    Candelas, X

    P. Candelas, X. C. De La Ossa, P. S. Green and L. Parkes,A Pair of Calabi-Yau manifolds as an exactly soluble superconformal theory,Nucl. Phys. B359(1991) 21

  22. [22]

    Mirror Symmetry for Two Parameter Models -- I

    P. Candelas, X. De La Ossa, A. Font, S. H. Katz and D. R. Morrison,Mirror symmetry for two parameter models. 1.,Nucl. Phys. B416(1994) 481 [hep-th/9308083]

  23. [23]

    Mirror Symmetry for Two Parameter Models -- II

    P. Candelas, A. Font, S. H. Katz and D. R. Morrison,Mirror symmetry for two parameter models. 2.,Nucl. Phys. B429(1994) 626 [hep-th/9403187]

  24. [24]

    Bastian, T

    B. Bastian, T. W. Grimm and D. van de Heisteeg,Modeling General Asymptotic Calabi–Yau Periods,Fortsch. Phys.73(2025) e70010 [2105.02232]

  25. [25]

    Bastian, D

    B. Bastian, D. van de Heisteeg and L. Schlechter,Beyond large complex structure: quantized periods and boundary data for one-modulus singularities,JHEP07(2024) 151 [2306.01059]. 44

  26. [26]

    On the Geometry of the String Landscape and the Swampland

    H. Ooguri and C. Vafa,On the Geometry of the String Landscape and the Swampland, Nucl. Phys.B766(2007) 21 [hep-th/0605264]

  27. [27]

    S.-J. Lee, W. Lerche and T. Weigand,Emergent strings from infinite distance limits, JHEP02(2022) 190 [1910.01135]

  28. [28]

    Marchesano and M

    F. Marchesano and M. Wiesner,Instantons and infinite distances,JHEP08(2019) 088 [1904.04848]

  29. [29]

    Baume, F

    F. Baume, F. Marchesano and M. Wiesner,Instanton Corrections and Emergent Strings,JHEP04(2020) 174 [1912.02218]

  30. [30]

    Supersymmetry Breaking and alpha'-Corrections to Flux Induced Potentials

    K. Becker, M. Becker, M. Haack and J. Louis,Supersymmetry breaking and alpha-prime corrections to flux induced potentials,JHEP06(2002) 060 [hep-th/0204254]

  31. [31]

    Kaehler Corrections for the Volume Modulus of Flux Compactifications

    G. von Gersdorff and A. Hebecker,Kahler corrections for the volume modulus of flux compactifications,Phys. Lett. B624(2005) 270 [hep-th/0507131]

  32. [32]

    M. Berg, M. Haack and B. Kors,String loop corrections to Kahler potentials in orientifolds,JHEP11(2005) 030 [hep-th/0508043]

  33. [33]

    M. Berg, M. Haack and E. Pajer,Jumping Through Loops: On Soft Terms from Large Volume Compactifications,JHEP09(2007) 031 [0704.0737]

  34. [34]

    M. Berg, M. Haack and J. U. Kang,One-Loop Kahler Metric of D-Branes at Angles, JHEP11(2012) 091 [1112.5156]

  35. [35]

    T. W. Grimm, R. Savelli and M. Weissenbacher,Onα ′ corrections in N=1 F-theory compactifications,Phys. Lett. B725(2013) 431 [1303.3317]

  36. [36]

    T. W. Grimm, J. Keitel, R. Savelli and M. Weissenbacher,From M-theory higher curvature terms toα ′ corrections in F-theory,Nucl. Phys. B903(2016) 325 [1312.1376]

  37. [37]

    M. Berg, M. Haack, J. U. Kang and S. Sj¨ ors,Towards the one-loop K¨ ahler metric of Calabi-Yau orientifolds,JHEP12(2014) 077 [1407.0027]

  38. [38]

    F-theory at order $\alpha'^3$

    R. Minasian, T. G. Pugh and R. Savelli,F-theory at orderα ′3,JHEP10(2015) 050 [1506.06756]

  39. [39]

    F-theory Vacua and $\alpha'$-Corrections

    M. Weissenbacher,F-theory vacua andα ′-corrections,JHEP04(2020) 032 [1901.04758]

  40. [40]

    Klaewer, S.-J

    D. Klaewer, S.-J. Lee, T. Weigand and M. Wiesner,Quantum corrections in 4dN= 1 infinite distance limits and the weak gravity conjecture,JHEP03(2021) 252 [2011.00024]

  41. [41]

    Cicoli, F

    M. Cicoli, F. Quevedo, R. Savelli, A. Schachner and R. Valandro,Systematics of theα’ expansion in F-theory,JHEP08(2021) 099 [2106.04592]

  42. [42]

    Wiesner,Light strings and strong coupling in F-theory,JHEP04(2023) 088 [2210.14238]

    M. Wiesner,Light strings and strong coupling in F-theory,JHEP04(2023) 088 [2210.14238]. 45

  43. [43]

    Cvetiˇ c and M

    M. Cvetiˇ c and M. Wiesner,Nonperturbative resolution of strong coupling singularities in 4D N=1 heterotic M-theory,Phys. Rev. D110(2024) 106008 [2408.12458]

  44. [44]

    G. F. Casas and M. Wiesner,Towards the Non-Perturbative Completion of 4d N=1 Effective Theories of Gravity,2510.23698

  45. [45]

    T. W. Grimm and J. Louis,The Effective action of N = 1 Calabi-Yau orientifolds,Nucl. Phys. B699(2004) 387 [hep-th/0403067]

  46. [46]

    T. W. Grimm,The Effective action of type II Calabi-Yau orientifolds,Fortsch. Phys.53 (2005) 1179 [hep-th/0507153]

  47. [47]

    Evidence for F-Theory

    C. Vafa,Evidence for F theory,Nucl. Phys. B469(1996) 403 [hep-th/9602022]

  48. [48]

    F-theory and Orientifolds

    A. Sen,F theory and orientifolds,Nucl. Phys. B475(1996) 562 [hep-th/9605150]

  49. [49]

    F-theoretic vs microscopic description of a conformal N=2 SYM theory

    M. Billo, L. Gallot, A. Lerda and I. Pesando,F-theoretic versus microscopic description of a conformal N=2 SYM theory,JHEP11(2010) 041 [1008.5240]

  50. [50]

    B. R. Greene, D. R. Morrison and M. R. Plesser,Mirror manifolds in higher dimension, Commun. Math. Phys.173(1995) 559 [hep-th/9402119]

  51. [51]

    Mirror Symmetry, N=1 Superpotentials and Tensionless Strings on Calabi-Yau Four-Folds

    P. Mayr,Mirror symmetry, N=1 superpotentials and tensionless strings on Calabi-Yau four folds,Nucl. Phys.B494(1997) 489 [hep-th/9610162]

  52. [52]

    Calabi-Yau fourfolds for M- and F-Theory compactifications

    A. Klemm, B. Lian, S. S. Roan and S.-T. Yau,Calabi-Yau fourfolds for M theory and F theory compactifications,Nucl. Phys. B518(1998) 515 [hep-th/9701023]

  53. [53]

    On N=1 4d Effective Couplings for F-theory and Heterotic Vacua

    H. Jockers, P. Mayr and J. Walcher,On N=1 4d Effective Couplings for F-theory and Heterotic Vacua,Adv. Theor. Math. Phys.14(2010) 1433 [0912.3265]

  54. [54]

    Conifold Transitions in M-theory on Calabi-Yau Fourfolds with Background Fluxes

    K. Intriligator, H. Jockers, P. Mayr, D. R. Morrison and M. R. Plesser,Conifold Transitions in M-theory on Calabi-Yau Fourfolds with Background Fluxes,Adv. Theor. Math. Phys.17(2013) 601 [1203.6662]

  55. [55]

    Quantum periods of Calabi-Yau fourfolds

    A. Gerhardus and H. Jockers,Quantum periods of Calabi–Yau fourfolds,Nucl. Phys. B 913(2016) 425 [1604.05325]

  56. [56]

    C. F. Cota, A. Klemm and T. Schimannek,Modular Amplitudes and Flux-Superpotentials on elliptic Calabi-Yau fourfolds,JHEP01(2018) 086 [1709.02820]

  57. [57]

    T. W. Grimm, C. Li and I. Valenzuela,Asymptotic Flux Compactifications and the Swampland,JHEP06(2020) 009 [1910.09549]

  58. [58]

    van de Heisteeg,Charting the complex structure landscape of F-theory,JHEP05 (2025) 150 [2404.03456]

    D. van de Heisteeg,Charting the complex structure landscape of F-theory,JHEP05 (2025) 150 [2404.03456]

  59. [59]

    T. W. Grimm and D. van de Heisteeg,Exact flux vacua, symmetries, and the structure of the landscape,JHEP01(2025) 005 [2404.12422]

  60. [60]

    Prepotential, Mirror Map and F-Theory on K3

    W. Lerche and S. Stieberger,Prepotential, mirror map and F theory on K3,Adv. Theor. Math. Phys.2(1998) 1105 [hep-th/9804176]. 46

  61. [61]

    On N=1 Mirror Symmetry for Open Type II Strings

    W. Lerche and P. Mayr,On N=1 mirror symmetry for open type 2 strings, hep-th/0111113

  62. [62]

    Holomorphic N=1 Special Geometry of Open--Closed Type II Strings

    W. Lerche, P. Mayr and N. Warner,Holomorphic N=1 special geometry of open - closed type II strings,hep-th/0207259

  63. [63]

    Effective superpotentials for compact D5-brane Calabi-Yau geometries

    H. Jockers and M. Soroush,Effective superpotentials for compact D5-brane Calabi-Yau geometries,Commun. Math. Phys.290(2009) 249 [0808.0761]

  64. [64]

    Relative periods and open-string integer invariants for a compact Calabi-Yau hypersurface

    H. Jockers and M. Soroush,Relative periods and open-string integer invariants for a compact Calabi-Yau hypersurface,Nucl. Phys. B821(2009) 535 [0904.4674]

  65. [65]

    M. Alim, M. Hecht, P. Mayr and A. Mertens,Mirror Symmetry for Toric Branes on Compact Hypersurfaces,JHEP09(2009) 126 [0901.2937]

  66. [66]

    M. Alim, M. Hecht, H. Jockers, P. Mayr, A. Mertens and M. Soroush,Hints for Off-Shell Mirror Symmetry in type II/F-theory Compactifications,Nucl. Phys. B841 (2010) 303 [0909.1842]

  67. [67]

    T. W. Grimm, T.-W. Ha, A. Klemm and D. Klevers,Computing Brane and Flux Superpotentials in F-theory Compactifications,JHEP04(2010) 015 [0909.2025]

  68. [68]

    M. Alim, M. Hecht, H. Jockers, P. Mayr, A. Mertens and M. Soroush,Type II/F-theory Superpotentials with Several Deformations and N=1 Mirror Symmetry,JHEP06(2011) 103 [1010.0977]

  69. [69]

    Lee and T

    S.-J. Lee and T. Weigand,Elliptic K3 surfaces at infinite complex structure and their refined Kulikov models,JHEP09(2022) 143 [2112.07682]

  70. [70]

    S.-J. Lee, W. Lerche and T. Weigand,Physics of infinite complex structure limits in eight dimensions,JHEP06(2022) 042 [2112.08385]

  71. [71]

    Cicoli, J.P

    M. Cicoli, J. P. Conlon, A. Maharana, S. Parameswaran, F. Quevedo and I. Zavala, String cosmology: From the early universe to today,Phys. Rept.1059(2024) 1 [2303.04819]

  72. [72]

    McAllister and A

    L. McAllister and A. Schachner,TASI Lectures on de Sitter Vacua,2512.17095

  73. [73]

    Four-dimensional String Compactifications with D-Branes, Orientifolds and Fluxes

    R. Blumenhagen, B. Kors, D. Lust and S. Stieberger,Four-dimensional String Compactifications with D-Branes, Orientifolds and Fluxes,Phys. Rept.445(2007) 1 [hep-th/0610327]

  74. [74]

    L. E. Ibanez and A. M. Uranga,String theory and particle physics: An introduction to string phenomenology. Cambridge University Press, 2, 2012

  75. [75]

    The Sen Limit

    A. Clingher, R. Donagi and M. Wijnholt,The Sen Limit,Adv. Theor. Math. Phys.18 (2014) 613 [1212.4505]

  76. [76]

    Bianchi and A

    M. Bianchi and A. Sagnotti,Twist symmetry and open string Wilson lines,Nucl. Phys. B361(1991) 519

  77. [77]

    E. G. Gimon and J. Polchinski,Consistency conditions for orientifolds and d manifolds, Phys. Rev.D54(1996) 1667 [hep-th/9601038]. 47

  78. [78]

    P. G. Camara and E. Dudas,Multi-instanton and string loop corrections in toroidal orbifold models,JHEP08(2008) 069 [0806.3102]

  79. [79]

    Mirror Symmetry is T-Duality

    A. Strominger, S.-T. Yau and E. Zaslow,Mirror symmetry is T duality,Nucl. Phys. B 479(1996) 243 [hep-th/9606040]

  80. [80]

    Enr´ ıquez Rojo and E

    M. Enr´ ıquez Rojo and E. Plauschinn,Swampland conjectures for type IIB orientifolds with closed-string U(1)s,JHEP07(2020) 026 [2002.04050]

Showing first 80 references.