2009
DOI: 10.1007/s00208-009-0406-9
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Modular forms of weight 8 for Γ g (1, 2)

Abstract: We complete the program indicated by the Ansatz of D'Hoker and Phong in genus 4 by proving the uniqueness of the restriction to Jacobians of the weight 8 Siegel cusp forms satisfying the Ansatz. We prove dim[ 4 (1, 2), 8] 0 = 2 and dim[ 4 (1, 2), 8] = 7. In each genus, we classify the linear relations among the selfdual lattices of rank 16. We extend the program to genus 5 by constructing the unique linear combination of theta series that satisfies the Ansatz.

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Cited by 15 publications
(52 citation statements)
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“…The OPSMY ansatz from [35] is constructed using lattice theta series, defined as follows for any lattice Λ ⊂ R n :…”
Section: For a Theta Characteristicmentioning
confidence: 99%
See 1 more Smart Citation
“…The OPSMY ansatz from [35] is constructed using lattice theta series, defined as follows for any lattice Λ ⊂ R n :…”
Section: For a Theta Characteristicmentioning
confidence: 99%
“…Then, the second ansatz was formulated in terms of theta series for 16-dimensional self-dual lattices by M. Oura, C. Poor,R. Salvati Manni and D. Yuen (OPSMY) in [35]. This second ansatz, however, is only defined for genera g ≤ 5.…”
Section: Introductionmentioning
confidence: 99%
“…This Ansatz can be satisfied through g ≤ 5 but is thought unlikely to extend further [18]. Over the hyperelliptic locus, however, the corresponding conditions are solved for all g by a family of binary invariants, see [19].…”
Section: An Applicationmentioning
confidence: 99%
“…For g > 5 some issues arise due to the presence of holomorphic roots of modular forms in the definition of the chiral measure, and it is not clear whether such roots are well defined and have the correct modular properties. In [14], Oura, Poor, Salvati Manni and Yuen (OPSMY) proposed an alternative construction for the chiral measure up to g = 5, using lattice theta series rather than theta constants, as done by Grushevsky. They also proved that the solution to the constraints is unique up to g = 4.…”
Section: Introductionmentioning
confidence: 99%
“…Another simple consequence is that the proposed three-point amplitude does not vanish at genus four as requested by the non-renormalisation theorem. We conclude this section by considering the OPSMY ansatz for the superstring measure in terms of theta lattices [14].…”
Section: Introductionmentioning
confidence: 99%