Pith. sign in

REVIEW 3 major objections 4 minor 110 references

Beyond Algebraic Superstring Compactification

T0 review · 3 major / 4 minor · reviewed 2026-08-08 · deepseek-v4-flash

Pith's one-line read The paper seeks to establish that Laurent-deformed Calabi-Yau hypersurfaces, completed by the intrinsic limit, are non-algebraic toric spaces carrying a maximal torus action and equivariant cohomology, and that transposition mirror…

desk verdict Honest conjecture-driven paper extending toric mirror symmetry to non-algebraic completions; the central step lacks a termination proof, but the explicit examples and framing deserve referee time. read the letter →

arxiv 2502.08002 v2 pith:EE3EXB2I submitted 2025-02-11 hep-th math.AG

classification hep-thmath.AG
keywords Calabi-YaucompactificationtoricgeometrymirrorsymmetryLaurentdeformationsintrinsiclimitHirzebruchscrollsVEXmultitopesequivariantcohomology
verification ladder T0 review T1 audit T2 compute T3 formal

The pith

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

The reading

The paper argues that superstring compactifications are not confined to complex algebraic varieties. Working with an infinite family of gauged linear $\sigma$ models whose ground states are Calabi-Yau hypersurfaces in Hirzebruch scrolls, it shows that 'unsmoothable' Tyurin-degenerate models can be smoothed by rational-monomial (Laurent) deformations. The zero loci of such deformed polynomials, completed by a constrained limiting procedure called the intrinsic limit, are claimed to be non-algebraic toric spaces equipped with a maximal $U(1)^n$ action and corresponding equivariant cohomology (Conjecture 2.1). It further claims that the transposition mirror construction extends to these spaces, yielding mirror pairs in which the mirror ambient space is assembled from flip-folded, multi-layered 'VEX multitopes' and may be only pre-complex rather than complex (Conjecture 3.1). If these claims hold, the Calabi-Yau landscape is far richer than the purely algebraic constructions catalogued over the past decades, and a $U(1)^n$-equivariant (co)homology theory is needed for computation.

What carries the argument

The central object is the intrinsic limit (Definition 2.1), a constrained limiting procedure that defines the closure of the zero locus of a Laurent-deformed polynomial by iterated L'Hôpital rule along the pole locus. The companion mechanism is the transpolar operation, a stripe-wise local dual mapping the Newton (multi)polytope of anticanonical monomials to the (multi)fan of the toric ambient space; unlike the standard global polar operation, it respects non-convexity and flip-folding. The combinatorial container is the VEX multitope (Definition 3.1): a continuously orientable, possibly multi-layered, multihedral body with every facet at unit distance from the origin, star-triangulated by a 0-centered multifan. The GLSM charge matrix and the deformation-distance poset of monomials generate the Mori vectors and the fan, making the entire construction computable by linear algebra.

What would settle it

A concrete Laurent-deformed hypersurface with a higher-order pole, such as a term $x_2^3/x_5^2$ in a higher-twist Hirzebruch scroll with $m\geq 3$, for which the intrinsic-limit iterations do not terminate, or for which two different orders of taking coordinate limits yield different completed zero loci, would disprove the well-definedness of the completion and thus Conjecture 2.1.

Watch

Extended reading notes

Core claim

The load-bearing assertion is Conjecture 2.1: Laurent-deformed Calabi-Yau hypersurfaces closed/completed by the 'intrinsic limit' are not algebraic varieties; they are toric spaces, equipped with a maximal $U(1)^n$-action, and corresponding $U(1)^n$- or even fully $U(1;\mathbb{C})^n$-equivariant (co)homology. The supporting construction is explicit: in the family $F^{(2)}_3$, the fundamental monomial admits rational deformations $x_2^2/x_5$ and $x_2^2/x_6$ that make the generic zero locus transverse, whereas regular polynomial deformations cannot. The intrinsic limit (Definition 2.1) resolves the pole ambiguity by a constrained L'Hôpital rule, and the paper proposes that the completed zero locus is a toric space whose combinatorial avatar is a VEX multitope closed under the transpolar involution. Mirror symmetry is then claimed to transpose this data: the mirror of a hypersurface in a non-Fano toric variety with non-convex spanning polytope is a transposed hypersurface in a flip-folded toric space (Conjecture 3.1), and the transpolar operation is conjectured to be an involution on VEX multitopes (Conjecture 3.2).

Load-bearing premise

The whole construction depends on the unproven assumption that the intrinsic-limit procedure terminates after finitely many steps and gives a unique completed zero locus, a point the paper flags in Remark 2.7.

Editorial extensions

If this is right

  • The Calabi-Yau landscape expands to include intrinsically non-algebraic toric spaces, so the standard algebraic-geometry toolkit for string compactification is insufficient.
  • Tyurin-degenerate Calabi-Yau hypersurfaces that are unsmoothable by regular polynomial deformations become transverse after Laurent deformations and intrinsic-limit completion, producing explicit smooth models in Hirzebruch scrolls.
  • Transposition mirror symmetry survives the passage to non-algebraic toric spaces, with mirror ambient spaces built from flip-folded multitopes and possibly pre-complex structures.
  • The combinatorial framework of VEX multitopes extends reflexive polytopes and the standard polar duality to non-convex, multi-layered objects, subsuming 'generalized legal loops' in all dimensions.
  • A $U(1)^n$- or $U(1;\mathbb{C})^n$-equivariant (co)homology theory is needed to compute the physical data, such as Betti and Hodge numbers and Yukawa couplings, of these compactifications.

Reading between the lines

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

  • The intrinsic limit, if proven to terminate, could be reinterpreted as a systematic desingularization-by-limits that may be equivalent to adding a divisor at infinity in a compactification; testing it on higher-order pole terms would reveal whether the completion is independent of the order of limits.
  • The 'blowout' phenomenon (a flip-folded subdivision with exceptional divisor of positive self-intersection) might correspond to exotic transitions in the Kähler moduli space, potentially realizing 'non-geometric' GLSM phases as honest geometric objects.
  • If Conjecture 2.2 holds, the entire deformation family could be smoothed by regular sections away from the Tyurin point, suggesting that Laurent deformations are limits of ordinary deformations and that the non-algebraic locus is a boundary component of the moduli space.
  • Homological mirror symmetry for these spaces would require an equivariant version of the derived category; the paper's proposal of $U(1;\mathbb{C})^n$-equivariant cohomology is a first step that could be checked by computing the equivariant cohomology ring of the completed $F^{(2)}_3$ example.
Share X Bluesky LinkedIn Reddit HN

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, and a circularity audit.

Referee Report

3 major / 4 minor

Summary. The paper argues that Laurent-deformed Calabi-Yau hypersurfaces, completed by a constrained 'intrinsic limit' procedure, are not algebraic varieties but toric spaces carrying a maximal U(1)^n action and equivariant (co)homology, and that transposition mirror symmetry extends to such spaces. The argument is built around an infinite family of Hirzebruch scrolls F_m^(n): the paper gives explicit charge matrices, monomial systems, fans, directrix sections, self-intersection computations, and a deformation path connecting F_5^(4), F_(4100)^(4), F_(3110)^(4), and F_(2111)^(4). It then introduces VEX multitopes, flip-folded multifans, and the transpolar operation as the combinatorial machinery for the mirror construction, and closes with an algebraic alternative via fractional changes of variables. The main claims are explicitly labeled as Conjectures 2.1, 2.2, 3.1, 3.2, and 4.1, with Remark 2.7 admitting that termination of the intrinsic limit is unproved.

Significance. If the conjectures are correct, the paper would open a genuinely new class of string compactification targets beyond algebraic Calabi-Yau varieties, with concrete computational tools and a mirror-symmetric organizational principle. The explicit charge matrices, Jacobian computations, self-intersection numbers, and the systematic deformation-family analysis are valuable and verifiable by inspection, and the paper is honest about the conjectural status of its central claims. The weaknesses are equally clear: the existence and uniqueness of the intrinsic-limit completion, which is the load-bearing step, is not proved, and the transpolar mirror construction for non-Fano examples relies on a prior unproved conjecture from the same program. The paper is best read as a programmatic proposal with strong computational motivation rather than as a completed mathematical or physical proof.

major comments (3)
  1. [§2.4, Definition 2.1 and Remark 2.7] The central object of Conjecture 2.1 depends on the intrinsic limit, but Definition 2.1 only specifies the constrained limit for the simple pole case (2.52)-(2.53). Remark 2.7 explicitly states that termination of the iterative L'Hopital procedure is not proved, and the paper gives no argument that the completion is independent of the order of limits or of the chosen path toward the pole locus, nor that the resulting object is finite-dimensional and carries the claimed maximal U(1)^n action. Since Conjecture 2.1 is the foundation for the subsequent mirror claims, this gap is load-bearing and needs to be addressed at least for the concrete families used here.
  2. [§3.3, eq. (3.4) and Conjecture 3.2] The mirror-space construction for the non-Fano example (3.4) uses the transpolar operation, whose closure and involutivity on VEX multitopes is Conjecture 3.2, taken from reference [62] of the same program. Consequently, the mirror-pair claim in (3.4) is not an independent check of the framework: it is contingent on an unproved conjecture about the very operation used to define the mirror. The paper should either provide a proof of Conjecture 3.2 in the cases needed here, or clearly state that the mirror identification is conditional on that conjecture.
  3. [§3.3, items 1-6] Conjecture 3.1 asserts the existence of a toric space ▽X encoded by a flip-folded spanning multitope, but the paper's own discussion shows that multifans do not uniquely determine torus manifolds (item 6), and that the gluing of the charts U23 # U34 and U34 # U41 in (3.5) is nonstandard. Without a well-defined space ▽F_m^(2), the statement that the transpose hypersurface Z_{f^T} lives in a toric space is not yet a well-posed claim. A concrete criterion or construction selecting the intended unitary torus manifold would be needed to make Conjecture 3.1 operational.
minor comments (4)
  1. [§3.3, VEX multitope paragraph] In the sentence following Definition 3.1, 'were ς ≺· σ is a facet' appears to contain typographical errors; it should presumably read 'where τ ≺ σ is a facet.'
  2. [§3.3, gluing discussion] The phrase 'but but requires much more detailed analysis' contains a duplicated 'but' and should be corrected.
  3. [§2.3, eqs. (2.33)-(2.33)] The cross-reference '(2.33)-(2.33)' is repeated; one occurrence should be corrected to the intended equation numbers for the directrices of F_(3110)^(4).
  4. [§2.4, eq. (2.51)] The display of the Laurent deformation terms in (2.51) uses 'x_5^k x_6^{m-2-k}' without parenthesizing the sum '(x_2⊕x_3⊕x_4)^4'; clarifying the intended grouping would improve readability.

Circularity Check

3 steps flagged · score 7.0 of 10

Non-algebraic mirror extension is built on the authors’ own unproved transpolar-involution conjecture (Conj. 3.2, Ref. [62]); intrinsic-limit completion is likewise admitted unproved.

  1. ansatz smuggled in via citation [§3.3, item 5 (Flip-Folded Layers); used in Conjectures 3.1 and 3.2]
    "This is a key characteristic of the “generalized legal loops” [99] — which in fact are the 2-dimensional so-called VEX multitopes [60–62], the latter defined so that the transpolar operation acts within their class and always as an involution."

    The transpolar involution is presented as a defining property of VEX multitopes, with a citation to the authors’ own [60–62], but Definition 3.1 in this paper contains no such involution theorem. Conjecture 3.2, also citing [62], still leaves (Δ▽)▽ = Δ as an open conjecture. Conjecture 3.1’s mirror space ▽X is defined by exactly this involution, so the paper’s non-algebraic mirror prediction depends on a self-cited ansatz rather than on an independently proved result.

  2. self citation load bearing [§3.3, Conjecture 3.2 and Conjecture 3.1]
    "Conjecture 3.2 (Ref. [62]) For an L-lattice VEX multitope, ∆ : (1) ∆▽ ⊂ L∨ R is a VEX multitope, and (2) (∆▽)▽ = ∆ : the transpolar operation (§ 2.1) closes on VEX multitopes as an involution."

    Conjecture 3.1 states that for a non-Fano X with non-convex spanning polytope, the transposition mirror is a hypersurface in a toric space ▽X whose spanning multitope satisfies Δ⋆(▽X) = (Δ⋆(▽X))▽ = Δ(X). That equality is part (2) of Conjecture 3.2, imported from Ref. [62] and unproved in the present paper. The central extension of mirror symmetry to the non-algebraic, flip-folded setting therefore rests on a self-cited conjecture, not on a derivation given here.

1 more flagged steps
  1. other [§2.4, Definition 2.1 and Remark 2.7; feeds Conjecture 2.1]
    "Although the pole locations will have a growing complexity and order in higher dimensions and higher “twist” (m) in F(n)m, it would seem that the “intrinsic limit” resolution of the ambiguity in defining the zero locus, Zf, i.e., specifying its closure is a well defined procedure with a guaranteed finite completion. However, I am not aware of a proof."

    This is a flagged limitation rather than a full circular reduction: Definition 2.1 is itself imported from Ref. [60], and Remark 2.7 concedes there is no proof that the intrinsic-limit completion terminates or is independent of the limiting path. Conjecture 2.1’s subject is exactly such intrinsic-limit-completed Laurent hypersurfaces, so the conjecture is conditional on an unproved, self-cited construction. I weigh this as load-bearing missing support for the paper’s central claim.

full rationale

Most of the paper’s algebraic-toric combinatorics—the GLSM charge data, the monomial ‘stripe’ analysis, the fan diagrams, and the deformation sequence (2.50)—is self-contained and does not reduce to its inputs. The ordinary Berglund–Hübsch transposition mirror for algebraic Calabi–Yau hypersurfaces has independent grounding in Refs. [55–58]. However, the genuinely novel non-algebraic extension is not independently derived. Conjecture 3.1 defines the mirror space ▽X through the transpolar involution (Δ▽)▽ = Δ, which is imported as Conjecture 3.2 from the authors’ own Ref. [62] and is not proved in this paper; §3.3 even describes VEX multitopes as ‘defined so that’ this involution holds, although Definition 3.1 does not prove it. Likewise, Conjecture 2.1 concerns zero loci completed by the ‘intrinsic limit,’ a construction taken from Ref. [60] and admitted in Remark 2.7 to lack a termination proof. These are load-bearing self-citations with explicitly acknowledged missing support. Because the central claims are honestly labeled conjectures, the paper does not force its conclusions by definition; but the derivation chain for its strongest claims terminates in the authors’ own unproved conjectures, giving a substantial circularity burden.

Assumptions & free parameters 0 free parameters · 4 assumptions · 3 invented entities

The paper's central claims depend on unproved assumptions that come from the author's own prior papers (transpolar involution, VEX multitope definitions) and on an explicitly unproved limiting procedure. No empirical fitting is involved, so there are no fitted free parameters.

assumptions (4)
  • ad hoc to paper Intrinsic limit procedure terminates with a finite completion
    Remark 2.7 admits 'I am not aware of a proof' of termination, yet Conjecture 2.1 depends on it.
  • ad hoc to paper Transpolar operation is an involution on VEX multitopes (Conjecture 3.2 of [62])
    The construction of the mirror space ▽F^(2)_m and the self-duality of VEX multitopes rely on this unproved conjecture from the authors' prior work.
  • standard math Standard toric geometry: Cox coordinates, fans, MPCP desingularization, Batyrev polar duality
    Invoked throughout §§2-3 from Refs [47-49, 92].
  • standard math Berglund-Hübsch transposition mirror symmetry for algebraic transverse hypersurfaces
    Base result [55] used as the starting point for the conjectural extension to non-algebraic spaces.
invented entities (3)
  • VEX multitope
    purpose: To formalize non-convex, flip-folded, multi-layered polytopes on which the transpolar operation is conjectured to be an involution
    Defined in the authors' prior work [60-62] and used as the foundation for Conjectures 2.1 and 3.2; no independent falsifiable prediction is offered.
  • flip-folded multifan
    purpose: To encode the conjectural non-algebraic toric mirror spaces such as ▽F^(2)_m
    Introduced via examples in §3.3; the paper states it remains to be determined how these correlate with existing combinatorial data, so there is no external evidence.
  • intrinsic-limit completed Laurent hypersurface
    purpose: To define the closure of zero loci of rational-monomial deformations, conjectured to be non-algebraic toric spaces
    Definition 2.1 and Conjecture 2.1; no proof of well-definedness or independent evidence of validity is provided.

how reviews work

0 comments
Cite this review

Pith. "Pith review of Beyond Algebraic Superstring Compactification." pith.science (2026). https://pith.science/paper/EE3EXB2I

@misc{pith2026250208002,
  author       = {Pith},
  title        = {Pith review of: Beyond Algebraic Superstring Compactification},
  year         = {2026},
  howpublished = {\url{https://pith.science/paper/EE3EXB2I}},
  note         = {Machine review of arXiv:2502.08002}
}
read the original abstract

Superstring compactifications have been vigorously studied for over four decades, and have flourished involving an active iterative feedback between physics and (complex) algebraic geometry. This led to an unprecedented wealth of constructions, virtually all of which are "purely" algebraic. Recent developments however indicate many more possibilities to be afforded by including certain generalizations that, at first glance at least, are not algebraic -- yet fit remarkably well within an overall mirror-symmetric framework and are surprisingly amenable to standard computational analysis upon certain mild but systematic modifications.

Discussion (0). Continue with ORCID to comment.

Reference graph

Works this paper leans on

110 extracted references · 34 canonical work pages

  1. [62]

    Chern characteristics and Todd–Hirzebruch identities for transpolar pairs of toric spaces,

    P. Berglund and T. H¨ ubsch, “Chern characteristics and Todd–Hirzebruch identities for transpolar pairs of toric spaces,” arXiv:2403.07139 [hep-th]

  2. [1]

    Nonlinear models in 2+ ǫ dimensions,

    D. H. Friedan, “Nonlinear models in 2+ ǫ dimensions,” Phys. Rev. Lett. 45 (1980) 1057

  3. [2]

    Nonlinear models in 2+ ǫ dimensions,

    D. H. Friedan, “Nonlinear models in 2+ ǫ dimensions,” Ann. Phys. 163 (1985) 318–419

  4. [3]

    Polchinski, String theory

    J. Polchinski, String theory. Vol. 1: An introduction to the bosonic string . Cambridge Monographs on Mathematical Physics. Cambridge University Press, Dec., 2 007

  5. [4]

    Polchinski, String theory

    J. Polchinski, String theory. Vol. 2: Superstring theory and beyond . Cambridge Monographs on Mathematical Physics. Cambridge University Press, Dec., 2007

  6. [5]

    Semiinfin ite cohomology and string theory ,

    I. B. Frenkel, H. Garland, and G. J. Zuckerman, “Semiinfin ite cohomology and string theory ,” Proc. Nat. Acad. Sci. 83 (1986) 8442

  7. [6]

    String theory as the kahler geometry of loop space,

    M. J. Bowick and S. G. Rajeev , “String theory as the kahler geometry of loop space,” Phys. Rev. Lett. 58 (1987) 535

  8. [7]

    The holomorphic geometry o f closed bosonic string theory and Diff S1/S1,

    M. J. Bowick and S. G. Rajeev , “The holomorphic geometry o f closed bosonic string theory and Diff S1/S1,” Nucl. Phys. B293 (1987) 348

Show all 110 references
  1. [8]

    The complex geometry of strin g theory and loop space,

    M. J. Bowick and S. Rajeev , “The complex geometry of strin g theory and loop space,” in Johns Hopkins Workshop on Current Problems in Particle Theory , Y.-S. Duan, G. Dom´ okos, and S. K¨ ovesi-Dom´ okos, eds. World Sci. Publishing, Singapore, July , 1987

  2. [9]

    Curvature of Superdiff S1/S1,

    P. Oh and P. Ramond, “Curvature of Superdiff S1/S1,” Phys. Lett. B195 (1987) 130–134

  3. [10]

    Th e superstring Diff S1/S1 and holomorphic geometry ,

    D. Harari, D. K. Hong, P. Ramond, and V. G. J. Rodgers, “Th e superstring Diff S1/S1 and holomorphic geometry ,”Nucl. Phys. B294 (1987) 556–572

  4. [11]

    Holomorphic structure of sup erstring vacua,

    K. Pilch and N. P. Warner , “Holomorphic structure of sup erstring vacua,” Class. Quant. Grav. 4 (1987) 1183

  5. [12]

    Anomalies and curvature i n complex geometry ,

    M. J. Bowick and S. G. Rajeev , “ Anomalies and curvature i n complex geometry ,” Nucl. Phys. B296 (1988) 1007–1033 . 9For string theory applications, this requires a (co)homolo gy theory consistent with mirror symmetry and conifold/geo metric transitions including various ass...

  6. [13]

    The Ricci curvature of diff S1/SL(2, R),

    M. J. Bowick and A. Lahiri, “The Ricci curvature of diff S1/SL(2, R),” J. Math. Phys. 29 (1988) 1979

  7. [14]

    String equations of motion from vanishing curvature,

    M. J. Bowick and K.-Q. Yang, “String equations of motion from vanishing curvature,” Int. J. Mod. Phys. A6 (1991) 1319–1334

  8. [15]

    H¨ ubsch,Calabi–Yau Manifolds: a Bestiary for Physicists

    T. H¨ ubsch,Calabi–Yau Manifolds: a Bestiary for Physicists . World Scientific Publishing Europe Ltd., London, UK, 2nd ed., 2024

  9. [16]

    Vacuum configurations for superstrings,

    P. Candelas, G. T. Horowitz, A. Strominger , and E. Witte n, “Vacuum configurations for superstrings,” Nucl. Phys. B258 (1985) 46–74

  10. [17]

    Sigma model beta functions and string compa ctifications,

    C. M. Hull, “Sigma model beta functions and string compa ctifications,” Nucl. Phys. B 267 (1986) 266–276

  11. [18]

    Superstrings with torsion,

    A. Strominger , “Superstrings with torsion,” Nucl. Phys. B 274 (1986) 253

  12. [19]

    Compactifications of the heterotic superst ring,

    C. M. Hull, “Compactifications of the heterotic superst ring,” Phys. Lett. B 178 (1986) 357–364

  13. [20]

    Torsional Heterotic Geometrie s,

    K. Becker and S. Sethi, “Torsional Heterotic Geometrie s,” Nucl. Phys. B 820 (2009) 1–31 , arXiv:0903.3769 [hep-th]

  14. [21]

    M theory , orienti folds and G - flux,

    K. Dasgupta, G. Rajesh, and S. Sethi, “M theory , orienti folds and G - flux,” JHEP 08 (1999) 023, arXiv:hep-th/9908088

  15. [22]

    Compactifications of heterotic strings on non-K¨ ahler complex manifolds. 2.,

    K. Becker , M. Becker , P. S. Green, K. Dasgupta, and E. Sha rpe, “Compactifications of heterotic strings on non-K¨ ahler complex manifolds. 2.,”Nucl. Phys. B678 (2004) 19–100 , arXiv:hep-th/0310058 [hep-th]

  16. [23]

    Comp actifications of heterotic theory on non-Kahler complex manifolds. 1.,

    K. Becker , M. Becker , K. Dasgupta, and P. S. Green, “Comp actifications of heterotic theory on non-Kahler complex manifolds. 1.,” JHEP 04 (2003) 007, arXiv:hep-th/0301161 [hep-th]

  17. [24]

    Phases of N = 2 theories in two-dimensions,

    E. Witten, “Phases of N = 2 theories in two-dimensions,” Nucl. Phys. B403 (1993) 159–222 , hep-th/9301042

  18. [25]

    Summing the instanton s: Quantum cohomology and mirror symmetry in toric varieties,

    D. R. Morrison and M. R. Plesser , “Summing the instanton s: Quantum cohomology and mirror symmetry in toric varieties,” Nucl. Phys. B440 (1995) 279–354 , arXiv:hep-th/9412236 [hep-th]

  19. [26]

    Calab i–Yau moduli space, mirror manifolds and space-time topology change in string theory ,

    P. S. Aspinwall, B. R. Greene, and D. R. Morrison, “Calab i–Yau moduli space, mirror manifolds and space-time topology change in string theory ,” Nucl. Phys. B416 (1994) 414–480 , arXiv:hep-th/9309097

  20. [27]

    On the geometry and homology o f certain simple stratified varieties,

    T. H¨ ubsch and A. Rahman, “On the geometry and homology o f certain simple stratified varieties,” J. Geom. Phys. 53 (2005) 31–48 , arXiv:math/0210394

  21. [28]

    Banagl, Intersection Spaces, Spatial Homology Truncation, and Str ing Theory

    M. Banagl, Intersection Spaces, Spatial Homology Truncation, and Str ing Theory. No. 1997 in Lecture Notes in Mathematics. Springer , 2010

  22. [29]

    Cobordism classes and the swam pland,

    J. McNamara and C. Vafa, “Cobordism classes and the swam pland,” arXiv:1909.10355 [hep-th]

  23. [30]

    On de Sitter spac etime and string theory ,

    P. Berglund, T. H¨ ubsch, and D. Minic, “On de Sitter spac etime and string theory ,” Int. J. Mod. Phys. D 32 no. 9, (Dec., 2023) 2330002 (111) , arXiv:2212.06086 [hep-th]

  24. [31]

    Finite representation of the solar gravita tional field in flat space of six dimensions,

    E. Kasner , “Finite representation of the solar gravita tional field in flat space of six dimensions,” American Journal of Mathematics 43 no. 2, (1921) 130–133 . http://www.jstor.org/stable/2370246

  25. [32]

    Completion and embedding of the Schwarzs child solution,

    C. Fronsdal, “Completion and embedding of the Schwarzs child solution,” Phys. Rev. 116 no. 3, (Nov , 1959) 778–781

  26. [33]

    (0, 2) Landau–Ginzburg theory ,

    J. Distler and S. Kachru, “ (0, 2) Landau–Ginzburg theory ,” Nucl. Phys. B 413 (1994) 213–243 , arXiv:hep-th/9309110

  27. [34]

    A survey of recent developments in GLSMs,

    E. Sharpe, “ A survey of recent developments in GLSMs,” Int. J. Mod. Phys. A 39 no. 33, (Jan., 2024) 2446001 , arXiv:2401.11637 [hep-th]

  28. [35]

    Complete classification of re flexive polyhedra in four-dimensions,

    M. Kreuzer and H. Skarke, “Complete classification of re flexive polyhedra in four-dimensions,” Adv. Theor . Math. Phys. 4 (2000) 1209–1230 , arXiv:hep-th/0002240

  29. [36]

    Calabi–Yau data

    M. Kreuzer and H. Skarke, “Calabi–Yau data.” 2000. http://hep.itp.tuwien.ac.at/~kreuzer/CY/. 22

  30. [37]

    Counting string theory standard models,

    A. Constantin, Y.-H. He, and A. Lukas, “Counting string theory standard models,” Phys. Lett. B 792 (2019) 258–262 , arXiv:1810.00444 [hep-th]

  31. [38]

    Calabi–Yau manifolds — motivations and co nstructions,

    T. H¨ ubsch, “Calabi–Yau manifolds — motivations and co nstructions,” Commun. Math. Phys. 108 (1987) 291–318

  32. [39]

    Calabi–Yau manifolds as com plete intersections in products of projective spaces,

    P. S. Green and T. H¨ ubsch, “Calabi–Yau manifolds as com plete intersections in products of projective spaces,” Comm. Math. Phys. 109 (1987) 99–108

  33. [40]

    Complete intersection Calabi–Yau manifolds,

    P. Candelas, A. M. Dale, C. A. L¨ utken, and R. Schimmrigk , “Complete intersection Calabi–Yau manifolds,” Nucl. Phys. B298 (1988) 493

  34. [41]

    Calabi–Yau manifolds in weighted P (4),

    P. Candelas, M. Lynker , and R. Schimmrigk, “Calabi–Yau manifolds in weighted P (4),” Nucl. Phys. B341 (1990) 383–402

  35. [42]

    On the classification of reflex ive polyhedra,

    M. Kreuzer and H. Skarke, “On the classification of reflex ive polyhedra,” Commun. Math. Phys. 185 (1997) 495–508 , arXiv:hep-th/9512204 [hep-th]

  36. [43]

    Weight systems for toric Calabi–Yau variet ies and reflexivity of Newton polyhedra,

    H. Skarke, “Weight systems for toric Calabi–Yau variet ies and reflexivity of Newton polyhedra,” Mod. Phys. Lett. A 11 no. 20, (Jun, 1996) 1637–1652 , arXiv:alg-geom/9603007 [alg-geom]

  37. [44]

    Classification of reflexive po lyhedra in three dimensions,

    M. Kreuzer and H. Skarke, “Classification of reflexive po lyhedra in three dimensions,” Adv. Theor . Math. Phys. 2 no. 4, (1998) 853 – 871 , arXiv:hep-th/9805190

  38. [45]

    Griffiths and J

    P. Griffiths and J. Harris, Principles of algebraic geometry . Wiley Classics Library . John Wiley & Sons Inc., New York, 1978

  39. [46]

    The geometry of toric varieties,

    V. I. Danilov , “The geometry of toric varieties,” Russian Math. Surveys 33 no. 2, (1978) 97–154 . http://stacks.iop.org/0036-0279/33/i=2/a=R03

  40. [47]

    Fulton, Introduction to T oric V arieties

    W. Fulton, Introduction to T oric V arieties. Annals of Mathematics Studies. Princeton University Pres s, 1993

  41. [48]

    Ewald, Combinatorial Convexity and Algebraic Geometry

    G. Ewald, Combinatorial Convexity and Algebraic Geometry . Springer Verlag, 1996

  42. [49]

    D. A. Cox, J. B. Little, and H. K. Schenck, T oric V arieties, vol. 124 of Graduate Studies in Mathematics . American Mathematical Society , 2011

  43. [50]

    Unidexter ous D = 2 supersymmetry in superspace,

    R. Brooks, F. Muhammad, and S. J. Gates, Jr ., “Unidexter ous D = 2 supersymmetry in superspace,” Nucl. Phys. B268 (1986) 599–620

  44. [51]

    Unidexterous D = 2 supersymmetry in superspace. 2. quantization,

    R. Brooks and S. J. Gates, Jr ., “Unidexterous D = 2 supersymmetry in superspace. 2. quantization,” Phys. Lett. B184 (1987) 217

  45. [52]

    Unidexter ous superspace: The flax of (super)strings,

    S. J. Gates, Jr ., R. Brooks, and F. Muhammad, “Unidexter ous superspace: The flax of (super)strings,” Phys. Lett. B194 (1987) 35

  46. [53]

    Calabi–Yau heterotic s trings and unidexterous sigma models,

    S. J. Gates, Jr . and T. H¨ ubsch, “Calabi–Yau heterotic s trings and unidexterous sigma models,” Nucl. Phys. B343 (1990) 741–774

  47. [54]

    Modern Approach to 2D Conformal Field Theor y,

    Y. Kusuki, “Modern Approach to 2D Conformal Field Theor y,” arXiv:2412.18307 [hep-th]

  48. [55]

    A generalized construction of mirror manifolds,

    P. Berglund and T. H¨ ubsch, “ A generalized construction of mirror manifolds,” Nucl. Phys. B393 no. 1-2, (1993) 377–391 , arXiv:hep-th/9201014 [hep-th] . [AMS/IP Stud. Adv . Math. 9 (1998) 327]

  49. [56]

    Landau–Ginzburg orbif olds, mirror symmetry and the elliptic genus,

    P. Berglund and M. Henningson, “Landau–Ginzburg orbif olds, mirror symmetry and the elliptic genus,” Nucl. Phys. B433 (1995) 311–332 , arXiv:hep-th/9401029 [hep-th]

  50. [57]

    FJRW-rings and mirror symmetry ,

    M. Krawitz, N. Priddis, P. Acosta, N. Bergin, and H. Rath nakumara, “FJRW-rings and mirror symmetry ,” Comm. Math. Phys. 296 no. 1, (Oct., 2009) 145–174 , arXiv:0903.3220 [math.AG]

  51. [58]

    Berglund-H¨ ubsch mirror symmetry via vertex algebras,

    L. A. Borisov , “Berglund-H¨ ubsch mirror symmetry via vertex algebras,” Comm. Math. Phys. 320 no. 1, (2013) 73–99 , arXiv:1007.2633 [math.AG] . 23

  52. [59]

    On Calabi–Yau generalized complete intersections from Hirzebruch varieties and novel K3-fibrations,

    P. Berglund and T. H¨ ubsch, “On Calabi–Yau generalized complete intersections from Hirzebruch varieties and novel K3-fibrations,” Adv. Theor . Math. Phys. 22 no. 2, (2018) 261 – 303 , arXiv:1606.07420 [hep-th]

  53. [60]

    A generalized construction of Calabi–Yau models and mirror symmetry ,

    P. Berglund and T. H¨ ubsch, “ A generalized construction of Calabi–Yau models and mirror symmetry ,” SciPost 4 no. 2, (2018) 009 (1–30) , arXiv:1611.10300 [hep-th]

  54. [61]

    Hirzebruch surfaces, Tyur in degenerations and toric mirrors: Bridging generalized Calabi–Yau constructions,

    P. Berglund and T. H¨ ubsch, “Hirzebruch surfaces, Tyur in degenerations and toric mirrors: Bridging generalized Calabi–Yau constructions,” Adv. Theor . Math. Phys. 26 no. 8, (2022) 2541–2598 , arXiv:2205.12827 [hep-th]

  55. [63]

    Ricci–flat mirror hypersurfaces in spaces of general type,

    T. H¨ ubsch, “Ricci–flat mirror hypersurfaces in spaces of general type,” in Proceedings of the 11th Mathematical Physics Meeting (Sep. 2–6. 2024) , B. Dragovich, ed. 2025. arXiv:2501.11684 [hep-th]

  56. [64]

    ¨Uber eine Klasse von einfach-zusammenh¨ angenden komplexen Mannigfaltigkeiten,

    F. Hirzebruch, “ ¨Uber eine Klasse von einfach-zusammenh¨ angenden komplexen Mannigfaltigkeiten,” Math. Ann. 124 (1951) 77–86

  57. [65]

    Unidexterous locally s upersymmetric actions for Calabi–Yau compactifications,

    S. J. Gates, Jr . and T. H¨ ubsch, “Unidexterous locally s upersymmetric actions for Calabi–Yau compactifications,” Phys. Lett. B226 (1989) 100

  58. [66]

    Chameleonic sigma-models,

    T. H¨ ubsch, “Chameleonic sigma-models,” Phys. Lett. B247 (1990) 317–322

  59. [67]

    How singular a space can superstrings thre ad?

    T. H¨ ubsch, “How singular a space can superstrings thre ad?” Mod. Phys. Lett. A6 (1991) 207–216

  60. [68]

    An SL(2,C) action on chiral rings and the mirror map,

    T. H¨ ubsch and S.-T. Yau, “ An SL(2,C) action on chiral rings and the mirror map,” Mod. Phys. Lett. A7 (1992) 3277–3289

  61. [69]

    Periods for Calabi–Yau and Landau–Ginzburg vacua,

    P. Berglund, P. Candelas, X. d. l. Ossa, A. Font, T. H¨ ubs ch, D. Jancic, and F. Quevedo, “Periods for Calabi–Yau and Landau–Ginzburg vacua,” Nucl. Phys. B419 (1994) 352–403 , arXiv:hep-th/9308005

  62. [70]

    Unitary toric manifolds, multi-fans and eq uivariant index,

    M. Masuda, “Unitary toric manifolds, multi-fans and eq uivariant index,” T ohoku Math. J. (2) 51 no. 2, (1999) 237–265 . http://projecteuclid.org/euclid.ojm/1178224815

  63. [71]

    From convex polytopes to multi-polytopes,

    M. Masuda, “From convex polytopes to multi-polytopes, ” Notes Res. Inst. Math. Analysis 1175 (2000) 1–15. http://hdl.handle.net/2433/64488

  64. [72]

    Theory of multi-fans,

    A. Hattori and M. Masuda, “Theory of multi-fans,” Osaka J. Math. 40 (2003) 1–68, arXiv:math/0106229 [math.SG] . http://projecteuclid.org/euclid.ojm/1153493035

  65. [73]

    On the cohomology of torus manif olds,

    M. Masuda and T. Panov , “On the cohomology of torus manif olds,” Osaka Journal of Mathematics 43 no. 3, (2006) 711 – 746 , arXiv:math/0306100 [math.AT]

  66. [74]

    Elliptic genera, torus manif olds and multi-fans,

    A. Hattori and M. Masuda, “Elliptic genera, torus manif olds and multi-fans,” Int. J. of Math. 16 no. 9, (July ,

  67. [75]

    Elliptic genera, torus orbifolds and mult i-fans; II,

    A. Hattori, “Elliptic genera, torus orbifolds and mult i-fans; II,” Int. J. Math 17 no. 06, (2006) 707–735 , arXiv:math/0501392 [math.AT]

  68. [76]

    Multipolytopes and convex chains,

    Y. Nishimura, “Multipolytopes and convex chains,” Proc. Steklov Inst. Math. 252 (2006) 212–224

  69. [77]

    Invariant stably complex structures on top ological toric manifolds,

    H. Ishida, “Invariant stably complex structures on top ological toric manifolds,” Osaka J. Math. 50 (2013) 795–806

  70. [78]

    Convex polytopes, Co xeter orbifolds and torus actions,

    M. W. Davis and T. Januszkiewicz, “Convex polytopes, Co xeter orbifolds and torus actions,” Duke Math. J. 62 no. 2, (1991) 417–451

  71. [79]

    Topological tor ic manifolds,

    H. Ishida, Y. Fukukawa, and M. Masuda, “Topological tor ic manifolds,” Moscow Math. J. 13 no. 1, (2013) 57–98 , arXiv:1012.1786 [math.AT]

  72. [80]

    Buchstaber and T

    V. Buchstaber and T. Panov , T oric T opology. No. 204 in Mathematical Surveys and Monographs. American Mathematical Society , Providence, RI, 2015. arXiv:1210.2368 [math.AT] . 24

  73. [81]

    Four dimensional almost complex torus manifo lds,

    D. Jang, “Four dimensional almost complex torus manifo lds,” arXiv:2310.11024 [math.DG]

  74. [82]

    On a residue representatio n of deformation, Koszul and chiral rings,

    P. Berglund and T. H¨ ubsch, “On a residue representatio n of deformation, Koszul and chiral rings,” Int. J. Mod. Phys. A 10 (1995) 3381–3430 , arXiv:hep-th/9411131

  75. [83]

    A pair of Calabi–Yau manifolds fro m a two parameter non-Abelian gauged linear sigma model,

    K. Hori and J. Knapp, “ A pair of Calabi–Yau manifolds fro m a two parameter non-Abelian gauged linear sigma model,” arXiv:1612.06214 [hep-th]

  76. [84]

    Nonabelian gauged linear sigma model,

    Y. Ruan, “Nonabelian gauged linear sigma model,” Chinese Annals of Mathematics, Series B 38 no. 4, (2017) 963–984 . https://doi.org/10.1007/s11401-017-1106-5

  77. [85]

    A new construction of Calabi–Yau manifolds: Generalized CICYs,

    L. B. Anderson, F. Apruzzi, X. Gao, J. Gray , and S.-J. Lee , “ A new construction of Calabi–Yau manifolds: Generalized CICYs,” Nucl. Phys. B906 (2016) 441–496 , arXiv:1507.03235 [hep-th]

  78. [86]

    A remark on generalize d complete intersections,

    A. Garbagnati and B. van Geemen, “ A remark on generalize d complete intersections,” Nucl. Phys. B925 (2017) 135–143 , arXiv:1708.00517 [math.AG]

  79. [87]

    Kodaira and D

    K. Kodaira and D. C. Spencer , On Deformations of Complex Analytic Structures . Princeton University , 1957

  80. [88]

    Classifications problems in differentia l topology V: On certain 6-manifolds,

    C. T. C. Wall, “Classifications problems in differentia l topology V: On certain 6-manifolds,” Invent. Math 1 (1966) 355–374

  81. [89]

    Complete K¨ ahler manifolds with zero Ricci curvature. I.,

    G. Tian and S.-T. Yau, “Complete K¨ ahler manifolds with zero Ricci curvature. I.,” J. Amer . Math. Soc. 3 no. 3, (1990) 579–609

  82. [90]

    Complete K¨ ahler manifolds with zero Ricci curvature. II.,

    G. Tian and S.-T. Yau, “Complete K¨ ahler manifolds with zero Ricci curvature. II.,” Invent. Math. 106 no. 1, (1991) 27–60

  83. [91]

    Duality in Calabi–Yau mo duli space,

    B. R. Greene and M. R. Plesser , “Duality in Calabi–Yau mo duli space,” Nucl. Phys. B338 (1990) 15–37

  84. [92]

    Dual polyhedra and mirror symmetry for C alabi–Yau hypersurfaces in toric varieties,

    V. V. Batyrev , “Dual polyhedra and mirror symmetry for C alabi–Yau hypersurfaces in toric varieties,” J. Alg. Geom. 3 no. 3, (1994) 493–535, arXiv:alg-geom/9310003

  85. [93]

    The homogeneous coordinate ring of a toric va riety ,

    D. A. Cox, “The homogeneous coordinate ring of a toric va riety ,”J. Algebraic Geometry 4 (1995) 17–50, arXiv:alg-geom/9210008 [alg-geom] . Erratum: J. Algebraic Geometry 23 (2014) 393-398

  86. [94]

    The moment map and line bundle s over presymplectic toric manifolds,

    Y. Karshon and S. Tolman, “The moment map and line bundle s over presymplectic toric manifolds,” J. Diff. Geom. 38 no. 3, (1993) 465–484 . https://projecteuclid.org/euclid.jdg/1214454478

  87. [95]

    Arnold, S

    V. Arnold, S. Gusein-Zade, and A. Varchenko, Singularities of Differentiable Maps , vol. 1. Birkh¨ auser , Boston, MA, 1985

  88. [96]

    Homological algebra of mirror symmetr y ,

    M. Kontsevich, “Homological algebra of mirror symmetr y ,” in International Congress of Mathematicians , S. D. Chatterji, ed., pp. 120–139. Birkh¨ auser Basel, Basel, 199 5. arXiv:alg-geom/9411018 [alg-geom]

  89. [97]

    Mirror symmetry in dimension 3,

    M. Kontsevich, “Mirror symmetry in dimension 3,” S´ eminaire Bourbaki (1994–95) exp. n◦ 801 in Ast´ erisque 237 (1996) 275–293. http://eudml.org/doc/110202

  90. [98]

    P. S. Aspinwall, T. Bridgeland, A. Craw , M. R. Douglas, A . Kapustin, G. W. Moore, M. Gross, G. Segal, B. Szendr˝ oi, and P. M. H. Wilson, Dirichlet branes and mirror symmetry , vol. 4 of Clay Mathematics Monographs. AMS, Providence, RI, 2009. http://people.maths.ox.ac.uk/cmi...

  91. [99]

    Lattice polygon s and the number 12,

    B. Poonen and F. Rodriguez-Villegas, “Lattice polygon s and the number 12,” Am. Math. Monthly 107 no. 3, (Mar ., 2000) 238–250

  92. [100]

    Huybrechts, Complex Geometry

    D. Huybrechts, Complex Geometry. Springer , 2005

  93. [101]

    A perverse sheaf approach toward a cohomol ogy theory for string theory ,

    A. Rahman, “ A perverse sheaf approach toward a cohomol ogy theory for string theory ,” Adv. Theor . Math. Phys. 13 no. 3, (2009) 667–693 , arXiv:0704.3298

  94. [102]

    Spec ial Lagrangian cycles and Calabi–Yau transitions,

    T. C. Collins, S. Gukov , S. Picard, and S.-T. Yau, “Spec ial Lagrangian cycles and Calabi–Yau transitions,” Comm. Math. Phys. 401 no. 1, (2023) 769–802 , arXiv:2111.10355 [math.DG] . 25

  95. [103]

    Branes and bu ndles through conifold transitions and dualities in heterotic string theory ,

    L. B. Anderson, C. R. Brodie, and J. Gray , “Branes and bu ndles through conifold transitions and dualities in heterotic string theory ,” Phys. Rev. D 108 no. 10, (2023) 106019, arXiv:2211.05804 [hep-th]

  96. [104]

    Gromov–Hausdorf f continuity of non-K¨ ahler Calabi–Yau conifold transitions,

    B. Friedman, S. Picard, and C. Suan, “Gromov–Hausdorf f continuity of non-K¨ ahler Calabi–Yau conifold transitions,” arXiv:2404.11840 [math.DG]

  97. [105]

    Calabi–Yau threefolds across quadratic s ingularities,

    S. Picard, “Calabi–Yau threefolds across quadratic s ingularities,” arXiv:2501.19313 [math.DG] . https://arxiv.org/abs/2501.19313

  98. [106]

    Star-shaped complexes and Ehrhart polynomi als,

    T. Hibi, “Star-shaped complexes and Ehrhart polynomi als,” Proc. Am. Math. Soc. 123 no. 3, (1995) 723–726

  99. [107]

    Kodaira, Complex Manifolds and Deformations of Complex Structures

    K. Kodaira, Complex Manifolds and Deformations of Complex Structures . Springer , New York, 1986

  100. [108]

    The moduli space of 3-folds with K = 0 may nevertheless be irreducible,

    M. A. Reid, “The moduli space of 3-folds with K = 0 may nevertheless be irreducible,” Math. Ann. 278 no. 1-4, (1987) 329–334

  101. [109]

    On threefolds with trivial canonical bundle,

    R. Friedman, “On threefolds with trivial canonical bundle,” in Complex Geometry and Lie Theory , J. A. Carlson, C. H. Clemens, and D. R. Morrison, eds., vol. 53, pp. 103–134. Amer . Math. Soc., Providence, RI, 1991. 26

  102. [2006]

    957–998, arXiv:math/0107014 [math.SG]

Pith tools

Reviewed August 8, 2026 · model on record in the stance chip above.