2002
DOI: 10.1142/s0129055x02001466
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Exceptional String: Instanton Expansions and Seiberg–witten Curve

Abstract: We investigate instanton expansions of partition functions of several toric Estring models using local mirror symmetry and elliptic modular forms. We also develop a method to determine the Seiberg-Witten curve of E-string with the help of elliptic functions.

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Cited by 26 publications
(56 citation statements)
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References 35 publications
(156 reference statements)
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“…Using these modified theta functions one can check easily using (3.12) that the elliptic genus of n M-strings, which is no longer holomorphic, satisfies the following holomorphic anomaly equation: 17) where ǫ + = ǫ 1 +ǫ 2 . Said differently, we are trading here the modular anomaly of (3.14) with the holomorphic anomaly of (3.17).…”
Section: M5mentioning
confidence: 99%
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“…Using these modified theta functions one can check easily using (3.12) that the elliptic genus of n M-strings, which is no longer holomorphic, satisfies the following holomorphic anomaly equation: 17) where ǫ + = ǫ 1 +ǫ 2 . Said differently, we are trading here the modular anomaly of (3.14) with the holomorphic anomaly of (3.17).…”
Section: M5mentioning
confidence: 99%
“…The free energy of a single E-string is known to arbitrary genus (see the discussion in Section 6.3); in the case of several strings, topological string techniques have been employed to compute the free energy to high genus (for instance, in [17] the free energy of up to five E-strings is computed up to g = 5). Recently, a similar approach was successfully developed [22] in the refined case (where ǫ 1 , ǫ 2 are taken to be arbitrary), generalizing techniques that were employed in the unrefined limit.…”
Section: -K3mentioning
confidence: 99%
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“…(1.1) as the six-dimensional Seiberg-Witten (SW) curve: the six-dimensional curve determines the prepotential of E-string theory and gives a complete description of its low-energy dynamics. Previously there were attempts at deriving the six-dimensional curve [4,5,6,7], however, only partial results with a few non-vanishing mass parameters {m i } were obtained. In this paper we will determine all the coefficient functions a j , b j and the curve (1.1) for arbitrary values of {m i }.…”
Section: Introductionmentioning
confidence: 99%
“…Among others, compactification down to four dimensions is of particular interest [4][5][6][7][8][9][10][11]. In this case, the low energy effective theory admits a description in terms of Seiberg-Witten theory [12,13].…”
Section: Introductionmentioning
confidence: 99%