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arxiv: 2604.28189 · v1 · submitted 2026-04-30 · ✦ hep-th · hep-ph

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Towards Systematics of Calabi-Yau Landscape for String Cosmology

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Pith reviewed 2026-05-07 05:57 UTC · model grok-4.3

classification ✦ hep-th hep-ph
keywords Calabi-Yau threefoldsmoduli stabilizationKKLTLVSfibre inflationstring cosmologyKähler conescalar potentials
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0 comments X

The pith

The topologies of divisors and curves in Calabi-Yau threefolds determine viable scalar potentials for moduli stabilization and inflation in string cosmology.

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

This review examines how the geometric features of Calabi-Yau threefolds influence the effective scalar potentials used in string theory models of cosmology. The authors explain that the shapes and connections of divisors and curves on these manifolds are essential for creating the right kinds of potentials in common stabilization methods like KKLT and LVS. They then focus on inflationary models within the LVS framework, particularly fibre inflation, and propose using multiple fibre moduli together to achieve sufficient inflation while staying within safe geometric limits. A sympathetic reader would care because this connects abstract string theory geometries directly to observable features of the early universe such as the duration of inflation. If correct, it provides a systematic way to select which Calabi-Yau spaces are suitable for building realistic cosmological models from string theory.

Core claim

The paper argues that the topologies of the various divisors and curves of the compactifying Calabi-Yau threefolds play a crucial role for generating the various suitable classes of effective scalar potentials within the framework of the popular moduli stabilization schemes such as KKLT and LVS. In the context of minimal LVS inflationary models such as fibre inflation, the specifics of the CY threefold geometries impact challenges such as the inflaton field-range bound. The authors discuss a multi-field approach in which several fibre moduli assist to drive successful inflation having a sufficient number of efolds without getting close to their individual Kähler cone boundaries.

What carries the argument

The topologies of divisors and curves on Calabi-Yau threefolds, which control the form of the effective scalar potential in moduli stabilization schemes like KKLT and LVS and enable multi-field fibre inflation.

If this is right

  • Suitable classes of effective scalar potentials for KKLT and LVS stabilization arise directly from the topologies of divisors and curves.
  • Multi-field fibre inflation within LVS can achieve a sufficient number of e-folds while respecting individual Kähler cone limits.
  • The inflaton field-range bound in single-field fibre inflation can be addressed by involving several fibre moduli together.
  • Global model building in string phenomenology gains a route to select CY geometries that support viable cosmological dynamics.

Where Pith is reading between the lines

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

  • This approach could guide computational searches for Calabi-Yau threefolds possessing multiple fibre structures suitable for inflation.
  • Cosmological measurements of inflation duration and spectral tilt might indirectly constrain the allowed topologies in the string landscape.
  • Extensions could examine whether the multi-field fibre mechanism remains stable when combined with other types of moduli.
  • Neighbouring problems include verifying that all non-fibre moduli stay stabilized throughout the multi-field inflationary phase.

Load-bearing premise

Specific Calabi-Yau threefolds exist with multiple fibre moduli that can be arranged into a viable multi-field inflationary trajectory staying inside the Kähler cone for enough e-folds while stabilizing remaining moduli.

What would settle it

A systematic search of known Calabi-Yau threefolds that fails to identify any with multiple fibre moduli capable of supporting multi-field inflation without violating Kähler cone boundaries or failing to stabilize other moduli.

read the original abstract

In this review, we discuss the relevance and impact of studying Calabi-Yau threefolds in the context of global model building in string phenomenology. First, taking a phenomenologist-friendly approach, we review how the topologies of the various divisors and curves of the compactifying CY threefolds play a crucial role for generating the various ``suitable" classes of effective scalar potentials, within the framework of the popular moduli stabilization schemes such as KKLT and LVS. Subsequently, we discuss the impact of the specifics of the CY threefold geometries in the minimal LVS inflationary models such as fibre inflation, in particular, along the challenges such as the inflaton field-range bound. In this regard, we discuss a multi-field approach in which several fibre moduli assist to drive successful inflation having a sufficient number of efolds, without getting close to their individual K\"ahler cone boundaries.

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 reviews how the topologies of divisors and curves in Calabi-Yau threefolds determine classes of effective scalar potentials within KKLT and LVS moduli stabilization. It examines the impact of CY geometry on minimal LVS inflationary models such as fibre inflation, focusing on the inflaton field-range bound, and proposes a multi-field approach in which several fibre moduli collectively drive inflation to achieve sufficient e-folds while remaining inside the Kähler cone.

Significance. The review usefully synthesizes the connection between CY threefold topology and viable effective potentials for string cosmology, drawing on established KKLT/LVS literature. The conceptual multi-field fibre inflation proposal could in principle address single-field field-range limitations, but its significance is limited by the absence of explicit geometric realizations or dynamical checks.

major comments (1)
  1. [multi-field approach discussion] The multi-field fibre inflation proposal (abstract and the section discussing the multi-field approach) rests on the assumption that suitable CY threefolds exist in which multiple fibre moduli produce a viable inflationary trajectory with N_e ≳ 60 that stays inside the Kähler cone and does not destabilize other moduli. No explicit example (e.g., a toric or hypersurface CY with h^{1,1} ≥ 3 containing multiple fibre divisors), no derived multi-field potential from the volume form and non-perturbative superpotential, and no numerical integration of the equations of motion are provided. This renders the central claim about generating sufficient e-folds without approaching Kähler cone boundaries conceptual rather than demonstrated.
minor comments (1)
  1. [Abstract] The abstract states that topologies 'play a crucial role for generating the various suitable classes of effective scalar potentials' but does not specify which topological invariants (e.g., intersection numbers, Euler characteristics of divisors) enter the potential at leading order; a brief enumeration in the introduction would improve clarity.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for their careful reading of the manuscript and for highlighting the conceptual nature of the multi-field fibre inflation proposal. We address this major comment below, clarifying the scope of the review and indicating the revisions we will make.

read point-by-point responses
  1. Referee: The multi-field fibre inflation proposal (abstract and the section discussing the multi-field approach) rests on the assumption that suitable CY threefolds exist in which multiple fibre moduli produce a viable inflationary trajectory with N_e ≳ 60 that stays inside the Kähler cone and does not destabilize other moduli. No explicit example (e.g., a toric or hypersurface CY with h^{1,1} ≥ 3 containing multiple fibre divisors), no derived multi-field potential from the volume form and non-perturbative superpotential, and no numerical integration of the equations of motion are provided. This renders the central claim about generating sufficient e-folds without approaching Kähler cone boundaries conceptual rather than demonstrated.

    Authors: We agree that the multi-field fibre inflation discussion is conceptual and does not provide an explicit Calabi-Yau realization, a derived multi-field potential, or numerical dynamical checks. The manuscript is a review whose primary aim is to connect divisor and curve topologies in Calabi-Yau threefolds to classes of effective potentials in KKLT and LVS scenarios, and then to examine the geometric constraints on minimal LVS inflationary models such as fibre inflation. Within that context, the multi-field approach is presented as a direction suggested by the topological analysis: several fibre moduli could collectively contribute to the inflaton trajectory, potentially allowing sufficient e-folds while remaining inside the Kähler cone. We do not assert that a concrete example has been constructed or verified in this work. To prevent any misinterpretation of the level of demonstration, we will revise the relevant section and abstract to state explicitly that this is a conceptual proposal motivated by the reviewed geometry, with explicit constructions and dynamical analysis left for future research. revision: partial

Circularity Check

0 steps flagged

No circularity: review builds on external KKLT/LVS literature with conceptual multi-field extension

full rationale

The paper is explicitly framed as a review discussing the established role of CY divisor/curve topologies in KKLT and LVS moduli stabilization (standard results from the broader literature) and then conceptually outlining a multi-field fibre inflation approach to address field-range bounds. No equations, fitted parameters, predictions, or derivations are presented that reduce by construction to inputs defined within the paper itself. The multi-field idea is described as a discussion/extension rather than a self-referential quantity or fitted output. All load-bearing elements rely on independently established external benchmarks, satisfying the criteria for a self-contained review with score 0.

Axiom & Free-Parameter Ledger

0 free parameters · 2 axioms · 0 invented entities

The central claims rest on standard domain assumptions of string compactification on Calabi-Yau threefolds and the validity of KKLT and LVS stabilization; no new free parameters, ad-hoc axioms, or invented entities are introduced in the abstract.

axioms (2)
  • domain assumption Calabi-Yau threefolds possess well-defined divisor and curve classes whose topologies determine the form of effective scalar potentials in moduli stabilization.
    Invoked when stating that topologies play a crucial role for generating suitable potentials in KKLT and LVS.
  • domain assumption KKLT and LVS are established and viable moduli stabilization schemes in type IIB string theory.
    Used as the framework throughout the review and for the fibre inflation discussion.

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Reference graph

Works this paper leans on

100 extracted references · 73 canonical work pages · 1 internal anchor

  1. [1]

    Green and T

    P. Green and T. Hubsch, Calabi-yau Manifolds as Complete Intersections in Products of Complex Projective Spaces,Commun. Math. Phys.109, 99 (1987). doi: 10.1007/BF01205673

  2. [2]

    Candelas, A

    P. Candelas, A. M. Dale, C. A. Lutken, and R. Schimmrigk, Complete Intersection Calabi-Yau Manifolds,Nucl. Phys. B.298, 493 (1988). doi: 10.1016/0550-3213(88)90352-5

  3. [3]

    P. S. Green, T. Hubsch, and C. A. Lutken, All Hodge Numbers of All Complete Intersection Calabi-Yau Manifolds,Class. Quant. Grav.6, 105– 124 (1989). doi: 10.1088/0264-9381/6/2/006

  4. [4]

    Candelas, X

    P. Candelas, X. De La Ossa, A. Font, S. H. Katz, and D. R. Morrison, Mirror symmetry for two parameter models. 1.,Nucl. Phys. B.416, 481– 538 (1994). doi: 10.1016/0550-3213(94)90322-0

  5. [5]

    V. V. Batyrev, Dual polyhedra and mirror symmetry for Calabi-Yau hyper- surfaces in toric varieties,J. Alg. Geom.3, 493–545 (1994)

  6. [6]

    Candelas, A

    P. Candelas, A. Font, S. H. Katz, and D. R. Morrison, Mirror symmetry for two parameter models. 2.,Nucl. Phys. B.429, 626–674 (1994). doi: 10.1016/0550-3213(94)90155-4

  7. [7]

    Hosono, A

    S. Hosono, A. Klemm, S. Theisen, and S.-T. Yau, Mirror symmetry, mirror map and applications to complete intersection Calabi-Yau spaces,Nucl. Phys. B.433, 501–554 (1995). doi: 10.1016/0550-3213(94)00440-P

  8. [8]

    Kreuzer and H

    M. Kreuzer and H. Skarke, Complete classification of reflexive polyhedra in four-dimensions,Adv. Theor. Math. Phys.4, 1209–1230 (2000). doi: 10. 4310/ATMP.2000.v4.n6.a2

  9. [9]

    J. Gray, A. S. Haupt, and A. Lukas, All Complete Intersection Calabi-Yau Four-Folds,JHEP.07, 070 (2013). doi: 10.1007/JHEP07(2013)070

  10. [10]

    L. B. Anderson, X. Gao, J. Gray, and S.-J. Lee, Fibrations in CICY Three- folds,JHEP.10, 077 (2017). doi: 10.1007/JHEP10(2017)077

  11. [11]

    L. B. Anderson, F. Apruzzi, X. Gao, J. Gray, and S.-J. Lee, A new con- struction of Calabi–Yau manifolds: Generalized CICYs,Nucl. Phys. B.906, 441–496 (2016). doi: 10.1016/j.nuclphysb.2016.03.016

  12. [12]

    JH EP 08, 109 (2021) https://doi.org/10.1007/JHEP08(2021)109 arXiv:2106.11964 [hep-th]

    M. Cicoli, I. n. G. Etxebarria, F. Quevedo, A. Schachner, P. Shukla, and R. Valandro, The Standard Model quiver in de Sitter string compactifica- tions,JHEP.08, 109 (2021). doi: 10.1007/JHEP08(2021)109

  13. [13]

    J. Gray, A. S. Haupt, and A. Lukas, Topological Invariants and Fibration Structure of Complete Intersection Calabi-Yau Four-Folds,JHEP.09, 093 20 (2014). doi: 10.1007/JHEP09(2014)093

  14. [14]

    L. B. Anderson, J. Gray, A. Lukas, and E. Palti, Two Hundred Heterotic Standard Models on Smooth Calabi-Yau Threefolds,Phys. Rev. D.84, 106005 (2011). doi: 10.1103/PhysRevD.84.106005

  15. [15]

    L. B. Anderson, J. Gray, A. Lukas, and E. Palti, Heterotic Line Bundle Standard Models,JHEP.06, 113 (2012). doi: 10.1007/JHEP06(2012)113

  16. [16]

    L. B. Anderson, A. Constantin, J. Gray, A. Lukas, and E. Palti, A Compre- hensive Scan for Heterotic SU(5) GUT models,JHEP.01, 047 (2014). doi: 10.1007/JHEP01(2014)047

  17. [17]

    L. B. Anderson, J. Gray, A. Lukas, and B. Ovrut, Stabilizing the Complex Structure in Heterotic Calabi-Yau Vacua,JHEP.02, 088 (2011). doi: 10. 1007/JHEP02(2011)088

  18. [18]

    L. B. Anderson, J. Gray, A. Lukas, and B. Ovrut, Stabilizing All Geometric Moduli in Heterotic Calabi-Yau Vacua,Phys. Rev. D.83, 106011 (2011). doi: 10.1103/PhysRevD.83.106011

  19. [19]

    Bobkov, V

    K. Bobkov, V. Braun, P. Kumar, and S. Raby, Stabilizing All Kahler Moduli in Type IIB Orientifolds,JHEP.12, 056 (2010). doi: 10.1007/ JHEP12(2010)056

  20. [20]

    Carta, A

    F. Carta, A. Mininno, N. Righi, and A. Westphal, Gopakumar-Vafa hi- erarchies in winding inflation and uplifts,JHEP.05, 271 (2021). doi: 10.1007/JHEP05(2021)271

  21. [21]

    Carta, A

    F. Carta, A. Mininno, N. Righi, and A. Westphal, Thraxions: Towards Full String Models (10, 2021)

  22. [22]

    Carta, A

    F. Carta, A. Mininno, and P. Shukla, Divisor topologies of CICY 3-folds and their applications to phenomenology,JHEP.05, 101 (2022). doi: 10. 1007/JHEP05(2022)101

  23. [23]

    Carta, A

    F. Carta, A. Mininno, and P. Shukla, Systematics of perturbatively flat flux vacua for CICYs (1, 2022)

  24. [24]

    Carta, J

    F. Carta, J. Moritz, and A. Westphal, A landscape of orientifold vacua, JHEP.05, 107 (2020). doi: 10.1007/JHEP05(2020)107

  25. [25]

    Gopakumar and C

    R. Gopakumar and C. Vafa, M theory and topological strings. 1. (9, 1998)

  26. [26]

    Gopakumar and C

    R. Gopakumar and C. Vafa, M theory and topological strings. 2. (12, 1998)

  27. [27]

    Kreuzer and H

    M. Kreuzer and H. Skarke, PALP: A Package for analyzing lattice polytopes with applications to toric geometry,Comput. Phys. Commun.157, 87–106 (2004). doi: 10.1016/S0010-4655(03)00491-0

  28. [28]

    A. P. Braun and N.-O. Walliser, A New offspring of PALP (6, 2011)

  29. [29]

    The Sage Developers.SageMath, the Sage Mathematics Software System (Version x.y.z)(YYYY).https://www.sagemath.org

  30. [30]

    Blumenhagen, B

    R. Blumenhagen, B. Jurke, T. Rahn, and H. Roschy, Cohomology of Line Bundles: A Computational Algorithm,J. Math. Phys.51, 103525 (2010). doi: 10.1063/1.3501132,10.1063/1.3523343

  31. [31]

    Blumenhagen, B

    R. Blumenhagen, B. Jurke, and T. Rahn, Computational Tools for Coho- mology of Toric Varieties,Adv. High Energy Phys.2011, 152749 (2011). doi: 10.1155/2011/152749

  32. [32]

    Altman, J

    R. Altman, J. Gray, Y.-H. He, V. Jejjala, and B. D. Nelson, A Calabi-Yau Database: Threefolds Constructed from the Kreuzer-Skarke List,JHEP. 21 02, 158 (2015). doi: 10.1007/JHEP02(2015)158

  33. [33]

    Altman, Y.-H

    R. Altman, Y.-H. He, V. Jejjala, and B. D. Nelson, New large volume Calabi-Yau threefolds,Phys. Rev. D.97(4), 046003 (2018). doi: 10.1103/ PhysRevD.97.046003

  34. [34]

    Cicoli, D

    M. Cicoli, D. Ciupke, C. Mayrhofer, and P. Shukla, A Geometrical Up- per Bound on the Inflaton Range,JHEP.05, 001 (2018). doi: 10.1007/ JHEP05(2018)001

  35. [35]

    Altman, J

    R. Altman, J. Carifio, X. Gao, and B. D. Nelson, Orientifold Calabi-Yau threefolds with divisor involutions and string landscape,JHEP.03, 087 (2022). doi: 10.1007/JHEP03(2022)087

  36. [36]

    Gao and P

    X. Gao and P. Shukla, On Classifying the Divisor Involutions in Calabi-Yau Threefolds,JHEP.1311, 170 (2013). doi: 10.1007/JHEP11(2013)170

  37. [37]

    Gao and H

    X. Gao and H. Zou, Machine Learning to the Orientifold Calabi-Yau with String Vacua (12, 2021)

  38. [38]

    Crin` o, F

    C. Crin` o, F. Quevedo, A. Schachner, and R. Valandro, A database of Calabi- Yau orientifolds and the size of D3-tadpoles,JHEP.08, 050 (2022). doi: 10.1007/JHEP08(2022)050

  39. [39]

    A. P. Braun, C. Long, L. McAllister, M. Stillman, and B. Sung, The Hodge Numbers of Divisors of Calabi-Yau Threefold Hypersurfaces (12, 2017)

  40. [40]

    Demirtas, C

    M. Demirtas, C. Long, L. McAllister, and M. Stillman, The Kreuzer-Skarke Axiverse,JHEP.04, 138 (2020). doi: 10.1007/JHEP04(2020)138

  41. [42]

    Gukov, C

    S. Gukov, C. Vafa, and E. Witten, CFT’s from Calabi-Yau four folds,Nucl. Phys.B584, 69–108 (2000). doi: 10.1016/S0550-3213(01)00289-9,10.1016/ S0550-3213(00)00373-4. [Erratum: Nucl. Phys.B608,477(2001)]

  42. [43]

    JHEP 06, 060 (2002) https://doi.org/10.1088/1126-6708/2002/06/060 arXiv:hep-th /0204254

    K. Becker, M. Becker, M. Haack, and J. Louis, Supersymmetry breaking and alpha-prime corrections to flux induced potentials,JHEP.06, 060 (2002). doi: 10.1088/1126-6708/2002/06/060

  43. [44]

    Witten, Nonperturbative superpotentials in string theory,Nucl

    E. Witten, Nonperturbative superpotentials in string theory,Nucl. Phys. B.474, 343–360 (1996). doi: 10.1016/0550-3213(96)00283-0

  44. [45]

    Bianchi, A

    M. Bianchi, A. Collinucci, and L. Martucci, Magnetized E3-brane instantons in F-theory,JHEP.12, 045 (2011). doi: 10.1007/JHEP12(2011)045

  45. [46]

    de Giorgi, M

    M. Bianchi, A. Collinucci, and L. Martucci, Freezing E3-brane instan- tons with fluxes,Fortsch. Phys.60, 914–920 (2012). doi: 10.1002/prop. 201200030

  46. [47]

    Louis, M

    J. Louis, M. Rummel, R. Valandro, and A. Westphal, Building an explicit de Sitter,JHEP.10, 163 (2012). doi: 10.1007/JHEP10(2012)163

  47. [48]

    JHEP 03, 007 (2005) https://doi.org/10.1088/1126-6708/2005/03/007 arXiv:hep-th /0502058

    V. Balasubramanian, P. Berglund, J. P. Conlon, and F. Quevedo, System- atics of moduli stabilisation in Calabi-Yau flux compactifications,JHEP. 03, 007 (2005). doi: 10.1088/1126-6708/2005/03/007

  48. [49]

    Antoniadis, Y

    I. Antoniadis, Y. Chen, and G. K. Leontaris, Perturbative moduli stabili- sation in type IIB/F-theory framework,Eur. Phys. J.C78(9), 766 (2018). doi: 10.1140/epjc/s10052-018-6248-4

  49. [50]

    Antoniadis, Y

    I. Antoniadis, Y. Chen, and G. K. Leontaris, Inflation from the internal 22 volume in type IIB/F-theory compactification,Int. J. Mod. Phys.A34(08), 1950042 (2019). doi: 10.1142/S0217751X19500428

  50. [51]

    Antoniadis, Y

    I. Antoniadis, Y. Chen, and G. K. Leontaris, Moduli stabilisation and infla- tion in type IIB/F-theory,PoS.CORFU2018, 068 (2019). doi: 10.22323/ 1.347.0068

  51. [52]

    Antoniadis, Y

    I. Antoniadis, Y. Chen, and G. K. Leontaris, Logarithmic loop corrections, moduli stabilisation and de Sitter vacua in string theory (2019)

  52. [53]

    Antoniadis, Y

    I. Antoniadis, Y. Chen, and G. K. Leontaris, String loop corrections and de Sitter vacua,PoS.CORFU2019, 099 (2020). doi: 10.22323/1.376.0099

  53. [54]

    Antoniadis, O

    I. Antoniadis, O. Lacombe, and G. K. Leontaris, Inflation near a metastable de Sitter vacuum from moduli stabilisation,Eur. Phys. J. C.80(11), 1014 (2020). doi: 10.1140/epjc/s10052-020-08581-9

  54. [55]

    G. K. Leontaris and P. Shukla, Stabilising all K¨ ahler moduli in perturbative LVS,JHEP.07, 047 (2022). doi: 10.1007/JHEP07(2022)047

  55. [56]

    Kachru, R

    S. Kachru, R. Kallosh, A. D. Linde, and S. P. Trivedi, De Sitter vacua in string theory,Phys. Rev.D68, 046005 (2003). doi: 10.1103/PhysRevD.68. 046005

  56. [57]

    Blumenhagen, A

    R. Blumenhagen, A. Collinucci, and B. Jurke, On Instanton Effects in F- theory,JHEP.08, 079 (2010). doi: 10.1007/JHEP08(2010)079

  57. [58]

    Cicoli, M

    M. Cicoli, M. Kreuzer, and C. Mayrhofer, Toric K3-Fibred Calabi-Yau Man- ifolds with del Pezzo Divisors for String Compactifications,JHEP.02, 002 (2012). doi: 10.1007/JHEP02(2012)002

  58. [59]

    JHEP 06, 162 (2012) https://doi.org/10.1007/JHEP06(2012)162 arXiv:1205.2485 [hep-th] 31

    R. Blumenhagen, X. Gao, T. Rahn, and P. Shukla, A Note on Poly- Instanton Effects in Type IIB Orientifolds on Calabi-Yau Threefolds,JHEP. 06, 162 (2012). doi: 10.1007/JHEP06(2012)162

  59. [60]

    Blumenhagen, X

    R. Blumenhagen, X. Gao, T. Rahn, and P. Shukla, Moduli Stabilization and Inflationary Cosmology with Poly-Instantons in Type IIB Orientifolds, JHEP.11, 101 (2012). doi: 10.1007/JHEP11(2012)101

  60. [61]

    and Burgess, C.P

    M. Cicoli, C. P. Burgess, and F. Quevedo, Fibre Inflation: Observable Grav- ity Waves from IIB String Compactifications,JCAP.0903, 013 (2009). doi: 10.1088/1475-7516/2009/03/013

  61. [62]

    Cicoli, F

    M. Cicoli, F. Muia, and P. Shukla, Global Embedding of Fibre Inflation Models,JHEP.11, 182 (2016). doi: 10.1007/JHEP11(2016)182

  62. [63]

    Cicoli, D

    M. Cicoli, D. Ciupke, V. A. Diaz, V. Guidetti, F. Muia, and P. Shukla, Chiral Global Embedding of Fibre Inflation Models,JHEP.11, 207 (2017). doi: 10.1007/JHEP11(2017)207

  63. [64]

    M. Berg, M. Haack, and B. Kors, String loop corrections to Kahler poten- tials in orientifolds,JHEP.11, 030 (2005). doi: 10.1088/1126-6708/2005/ 11/030

  64. [65]

    M. Berg, M. Haack, and E. Pajer, Jumping Through Loops: On Soft Terms from Large Volume Compactifications,JHEP.09, 031 (2007). doi: 10.1088/ 1126-6708/2007/09/031

  65. [66]

    JHEP 01, 052 (2008) https://doi.org/10.1088/1126-6708/2008/01/052 arXiv:0708.18 73 [hep-th]

    M. Cicoli, J. P. Conlon, and F. Quevedo, Systematics of String Loop Cor- rections in Type IIB Calabi-Yau Flux Compactifications,JHEP.01, 052 (2008). doi: 10.1088/1126-6708/2008/01/052

  66. [67]

    von Gersdorff and A

    G. von Gersdorff and A. Hebecker, Kahler corrections for the volume mod- 23 ulus of flux compactifications,Phys. Lett. B.624, 270–274 (2005). doi: 10.1016/j.physletb.2005.08.024

  67. [68]

    X. Gao, A. Hebecker, S. Schreyer, and G. Venken, Loops, local corrections and warping in the LVS and other type IIB models,JHEP.09, 091 (2022). doi: 10.1007/JHEP09(2022)091

  68. [69]

    Ciupke, J

    D. Ciupke, J. Louis, and A. Westphal, Higher-Derivative Supergravity and Moduli Stabilization,JHEP.10, 094 (2015). doi: 10.1007/JHEP10(2015) 094

  69. [70]

    JHEP 02, 062 (2012) https://doi.org/10.1007/JHEP02(2012)062 arXiv:1110.3333 [hep-th]

    M. Cicoli, C. Mayrhofer, and R. Valandro, Moduli Stabilisation for Chiral Global Models,JHEP.02, 062 (2012). doi: 10.1007/JHEP02(2012)062

  70. [71]

    JHEP 05, 001 (2014) https://doi.org/10.1007/JHEP05(2014)001 arXiv:1312.0014 [hep- th]

    M. Cicoli, D. Klevers, S. Krippendorf, C. Mayrhofer, F. Quevedo, and R. Va- landro, Explicit de Sitter Flux Vacua for Global String Models with Chiral Matter,JHEP.05, 001 (2014). doi: 10.1007/JHEP05(2014)001

  71. [72]

    Shukla, Classifying divisor topologies for string phenomenology,JHEP

    P. Shukla, Classifying divisor topologies for string phenomenology,JHEP. 12, 055 (2022). doi: 10.1007/JHEP12(2022)055

  72. [73]

    Blumenhagen, V

    R. Blumenhagen, V. Braun, T. W. Grimm, and T. Weigand, GUTs in Type IIB Orientifold Compactifications,Nucl.Phys.B815, 1–94 (2009). doi: 10.1016/j.nuclphysb.2009.02.011

  73. [74]

    Collinucci, M

    A. Collinucci, M. Kreuzer, C. Mayrhofer, and N.-O. Walliser, Four- modulus ’Swiss Cheese’ chiral models,JHEP.07, 074 (2009). doi: 10.1088/ 1126-6708/2009/07/074

  74. [75]

    Cicoli, M

    M. Cicoli, M. Licheri, P. Piantadosi, F. Quevedo, and P. Shukla, Higher derivative corrections to string inflation,JHEP.02, 115 (2024). doi: 10. 1007/JHEP02(2024)115

  75. [76]

    J. P. Conlon, F. Quevedo, and K. Suruliz, Large-volume flux compactifica- tions: Moduli spectrum and D3/D7 soft supersymmetry breaking,JHEP. 08, 007 (2005). doi: 10.1088/1126-6708/2005/08/007

  76. [77]

    J. J. Blanco-Pillado, D. Buck, E. J. Copeland, M. Gomez-Reino, and N. J. Nunes, Kahler Moduli Inflation Revisited,JHEP.01, 081 (2010). doi: 10. 1007/JHEP01(2010)081

  77. [78]

    Cicoli, I

    M. Cicoli, I. Garc` ıa-Etxebarria, C. Mayrhofer, F. Quevedo, P. Shukla, and R. Valandro, Global Orientifolded Quivers with Inflation,JHEP.11, 134 (2017). doi: 10.1007/JHEP11(2017)134

  78. [79]

    JHEP 09, 026 (2016) https://doi.org/10.1007/JHEP09(2016)026 arXiv:1607.01395 [hep-th]

    M. Cicoli, D. Ciupke, S. de Alwis, and F. Muia,α ′ Inflation: moduli sta- bilisation and observable tensors from higher derivatives,JHEP.09, 026 (2016). doi: 10.1007/JHEP09(2016)026

  79. [80]

    Cicoli, A

    M. Cicoli, A. Grassi, O. Lacombe, and F. G. Pedro, Chiral global embedding of Fibre Inflation with D3 uplift,JHEP.06, 090 (2025). doi: 10.1007/ JHEP06(2025)090

  80. [81]

    JCAP 12, 022 (2011) https://doi.org/10.1088/1475-7516/2011/12/022 arXiv:1110.61 82 [hep- th]

    M. Cicoli, F. G. Pedro, and G. Tasinato, Poly-instanton Inflation,JCAP. 12, 022 (2011). doi: 10.1088/1475-7516/2011/12/022

Showing first 80 references.