1996
DOI: 10.1007/bf02099367
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Arithmetic properties of mirror map and quantum coupling

Abstract: We study some arithmetic properties of the mirror maps and the quantum Yukawa coupling for some 1-parameter deformations of Calabi-Yau manifolds. First we use the Schwarzian differential equation, which we derived previously, to characterize the mirror map in each case. For algebraic K3 surfaces, we solve the equation in terms of the J-function. By deriving explicit modular relations we prove that some K3 mirror maps are algebraic over the genus zero function field Q(J). This leads to a uniform proof that thos… Show more

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Cited by 109 publications
(179 citation statements)
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References 18 publications
(69 reference statements)
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“…These number theoretic functions are also associated with topological c = 3 Landau-Ginzburg models [104,105] and certain superconformal quantum field theories [106]. In addition, the special class of Chebyshev models also has an interesting geometric interpretation in terms of mirror maps in weighted projective spaces [108][109][110][111][112][113]. These correspond to the normal forms of functions with unimodular singularities [114].…”
Section: Jhep05(2017)087mentioning
confidence: 99%
See 2 more Smart Citations
“…These number theoretic functions are also associated with topological c = 3 Landau-Ginzburg models [104,105] and certain superconformal quantum field theories [106]. In addition, the special class of Chebyshev models also has an interesting geometric interpretation in terms of mirror maps in weighted projective spaces [108][109][110][111][112][113]. These correspond to the normal forms of functions with unimodular singularities [114].…”
Section: Jhep05(2017)087mentioning
confidence: 99%
“…Indeed, it is well known [107] that ratios of solutions to the hypergeometric equation describe conformal maps of spherical triangles. These form the simplest nontrivial example of a mirror map [108][109][110][111][112]:…”
Section: Chebyshev Potentials and Mirror Curvesmentioning
confidence: 99%
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“…We proceed as before with a matrix that is now The null space of the matrix is two dimensional and we need to choose in this space a basis for the Mori cone. It is straightforward to do this in terms of combinatorial properties of the matrix however since this is not our main interest we can guess the answer by examining the large complex structure coordinates which for this case are λ = − 2φ (8ψ) 4 and µ = 1 (2φ) 2 .…”
Section: The Mirror Of the Octicmentioning
confidence: 99%
“…The large complex structure limit is the limit ψ, ℑ(t) → ∞ and in this limit the exponential terms, which express the quantum corrections, tend to zero and y ttt (ψ) → 5, the classical value. On the other hand it has been shown [4] that 5 3 |n k k 3 for each k so that we can in fact write…”
Section: Introductionmentioning
confidence: 99%