“…The Fourier coefficients of cusp forms are interesting and mysterious objects (see e.g. [5], [17], [14]). From the theory of Hecke operators, it is well known that λ f (n) is real and satisfies the multiplicative property…”
“…The Fourier coefficients of cusp forms are interesting and mysterious objects (see e.g. [5], [17], [14]). From the theory of Hecke operators, it is well known that λ f (n) is real and satisfies the multiplicative property…”
“…The main idea for our improvement is an alternative expression of G (s) in Lemma 2.1 below, different from [15,16,17,13]; this expression decomposes G (s) into a product of L-functions, general and (more importantly) of lower degree ( 3). Hence we can take advantage of their (individual or averaged) subconvexity bounds (see…”
In this paper, we investigate the th power sum of Hecke eigenvalues of classical holomorphic cusp forms for 3 8 and improve the related results of Lü [15, 16, 17]. We also establish Ω-estimates for 2 6 and affirm a conjecture of Ivić [7, (7.23)].
“…Later, Lau and Lü [8] generalized the above results to Maass cusp forms φ for SL (2, Z) and also to higher symmetric powers of φ, under the assumption that the higher symmetric powers are automorphic.…”
Section: Introductionmentioning
confidence: 88%
“…Now, we want to choose η 1 , η 2 > 0 to optimize the bound in (8). First we choose η 1 so that the first two terms on the right hand side of (8) are equal.…”
Let π be an irreducible cuspidal automorphic representation of GL(r, A) where r ≥ 2 and A is the adele ring of Q. Let a π (n) denote the nth Dirichlet series coefficient of the L-function associated to π. The main goal of this paper is to obtain strong bounds for the first moment n≤x a π (n) as x → ∞. The bounds we obtain are better than all previously obtained bounds for the higher rank situation when r ≥ 3 and π is not a symmetric power of a GL(2, A) cuspidal automorphic representation.
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