On modular forms associated with indefinite quadratic forms of signature (2,n?2) (original) (raw)
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1997
We start with a brief overview of the necessary theory: Given any cusp form f=∑ n≥ 1 an (f) qn of weight k, we denote by L (f, s) the L-function of f. For Re (s)> k/2+ 1, the value of L (f, s) is given by L (f, s)=∑ n≥ 1 an (f) ns and, one can show that L (f, s) has analytic continuation to the entire complex plane. The value of L (f, s) at s= k/2 will be of particular interest to us, and we will refer to this value as the central critical value of L (f, s).
2016
Let F be a totally real field and χ an abelian totally odd character of F. In 1988, Gross stated a p-adic analogue of Stark's conjecture that relates the value of the derivative of the p-adic L-function associated to χ and the p-adic logarithm of a p-unit in the extension of F cut out by χ. In this paper we prove Gross's conjecture when F is a real quadratic field and χ is a narrow ring class character. The main result also applies to general totally real fields for which Leopoldt's conjecture holds, assuming that either there are at least two primes above p in F , or that a certain condition relating the L-invariants of χ and χ −1 holds. This condition on L-invariants is always satisfied when χ is quadratic. Contents S. DASGUPTA, H. DARMON, and R. POLLACK 4. Galois representations 477 4.1. Representations attached to ordinary eigenforms 477 4.2. Construction of a cocycle 480 References 482
On generalized modular forms and their applications
Nagoya Math. J, 2008
Abstract. We study the Fourier coefficients of generalized modular forms f(τ) of integral weight k on subgroups Γ of finite index in the modular group. We establish two Theorems asserting that f(τ) is constant if k = 0, f(τ) has empty divisor, and the Fourier coefficients have certain ...
2-ADIC Properties of Certain Modular Forms and Their Applications to Arithmetic Functions
It is a classical observation of Serre that the Hecke algebra acts locally nilpo- tently on the graded ring of modular forms modulo 2 for the full modular group. Here we consider the problem of classifying spaces of modular forms for which this phenomenon continues to hold. We give a number of consequences of this investigation as they relate to quadratic forms, partition functions, and central values of twisted modular L-functions.
Acta Arithmetica, 1999
Dedicated to the memory of my greatest teachers, my parents, Thereza de Azevedo Pribitkin and Edmund Pribitkin 1. Historical introduction. In 1989 Knopp [6] found explicit formulas for the Fourier coefficients of an arbitrary cusp form and more generally, but conditionally, of a holomorphic modular form (with a possible pole at i∞) on the full modular group, Γ (1), of weight k, 4/3 < k < 2, and multiplier system v. He assumed that there are no nontrivial cusp forms on Γ (1) of complementary weight 2−k and conjugate multiplier system v. In our initial paper we remove this assumption and capture the Fourier coefficients of an arbitrary "Niebur modular integral" on Γ (1) of weight k, 1 < k < 2. En route we also obtain expressions for the Fourier coefficients of an arbitrary cusp form on Γ (1) of weight k, 0 < k < 1. In particular we present formulas for the Fourier coefficients of η r (τ), 0 < r < 2, where η(τ) is the Dedekind eta-function. An actual formula for the Fourier coefficients of an arbitrary modular form, even in the case of the full modular group, is not always available. For forms of weight greater than two the problem was solved by Petersson [11], who introduced the (parabolic) Poincaré series. Additionally, by considering a nonanalytic version of this series, he derived the coefficients of certain forms of weight two [12]. By integrating one of these forms, Petersson [12, p. 202] was the first to find the coefficients of the absolute modular invariant J(τ). For forms of negative weight Rademacher and Zuckerman [18] discovered expressions for the coefficients by relying on the circle method. Furthermore, Rademacher [15] employed a sharpened version of this method to rediscover Petersson's formula for J(τ). We remark that both approaches