Abstract
Let
where
1 Introduction
Let
It is known that
where
From Kim and Sarnak [1] and Sarnak [2] we know that
From [3], the Rankin-Selberg theory shows that
Due to
also holds, where
As in [4] and [5], the Godement-Jacquet L-function associated with
This L-function has a standard functional equation and analytic continuation to an entire function on complex plane
Then the L-function associated with the dual Maass form
We write
where the
In this paper, we focus our attention on the Hecke-Maass eigenforms for the group
Theorem 1
Let
From Theorem 1 we can get the following corollary immediately.
Corollary
We have
Remark
Due to the fact that
which implies
Thus, we restrict the range of
As applications of Theorem 1, we can establish the asymptotic formulas for the second, fourth and sixth powers of
Theorem 2
For any
where
Notation. Throughout this paper, the letter
2 Some lemmas
In order to prove Theorems 1 and 2, we first introduce some lemmas.
Lemma 2.1
Let
Proof
The proof of this lemma is similar to [27, Lemma 7.1], and we just need to use the following functional equation:
where
in place of the functional equation of
Lemma 2.2
For
is equivalent to
where
Proof
Let
where
And then replacing
which implies (2.1).□
Lemma 2.3
We suppose that
where for
which is equivalent to
Proof
We suppose that (2.6) is true and let
Then from (2.6) we have
thus for
Inversely, we let (2.4) hold and denote by
For each
□
Lemma 2.4
Let
where
where
Proof
We can get this lemma by following a similar argument to [6, Lemma 8.2] replacing
Lemma 2.5
[27, Theorem 5.2] Let
and the above formula remains also valid if
Lemma 2.6
[28, Corollary 1.2] Let
Lemma 2.7
For any
Proof
The first result is a general result of Perelli [26], which we can also get from Lemma 2.5 with
Lemma 2.8
For
Proof
Following a similar argument of Lemma 2.2, with the help of Lemma 2.7 we can obtain this lemma.□
Lemma 2.9
[27, Lemma 8.3] Let
In the following two lemmas, though the definitions of
Lemma 2.10
Let
Then we have
Lemma 2.11
Let
Then we have
3 Proofs of Theorems 1 and 2
3.1 Proof of Theorem 1
In this section, we restrict the range of
Recalling Mellin’s formula
Taking
Shifting the line of integration in (3.2) to
The integral part of (3.3) for which
Combining (2.5) with (3.4), we can obtain
or
where
For convenience, denote by
Recalling (1.1), we know that Lemma 2.4 is valid. We first consider
While for
and
For (3.8), if we take
For (3.9), if we take
Therefore, combining (3.10) with (3.11) we have
We assume that the second and the third terms in (3.12) do not exceed
Thus, we have
with
For
Recalling the value of
Thus, we complete the proof of Theorem 1.
3.2 Proof of Theorem 2
In this section, we give the proof of Theorem 2 by following a similar argument to [6, Theorem 2]. Let
holds for any
Writing
where
Combining Abel’s summation formula with Lemmas 2.5 and 2.10, we can obtain
Let
And applying Lemma 2.9 with
and
Recalling the definition of
Moreover,
where
By Lemma 2.5, Lemma 2.10 and Hölder’s inequality, we can obtain
Thus, Lemma 2.9 shows
Note that
holds for any
Thus,
and for fixed
From Theorem 1 we have
Recalling the definition of
Acknowledgment
The authors are greatly indebted to the reviewers for very beneficial suggestions and comments which led to essential improvement of the original version of this paper. This work was supported by the National Natural Science Foundation of China (Grant Nos. 11771256 and 11801328).
-
Conflict of interest: Authors state no conflict of interest.
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© 2021 Jing Huang et al., published by De Gruyter
This work is licensed under the Creative Commons Attribution 4.0 International License.
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- Special Issue on Boundary Value Problems and their Applications on Biosciences and Engineering (Part I)
- Marangoni convection in layers of water-based nanofluids under the effect of rotation
- A transient analysis to the M(τ)/M(τ)/k queue with time-dependent parameters
- Existence of random attractors and the upper semicontinuity for small random perturbations of 2D Navier-Stokes equations with linear damping
- Degenerate binomial and Poisson random variables associated with degenerate Lah-Bell polynomials
- Special Issue on Fractional Problems with Variable-Order or Variable Exponents (Part I)
- On the mixed fractional quantum and Hadamard derivatives for impulsive boundary value problems
- The Lp dual Minkowski problem about 0 < p < 1 and q > 0