1 Introduction
Dirichlet L-functions are fundamental objects in analytic number theory. Their extreme values are closely connected with several important problems, including estimates for character sums, the distribution of quadratic residues and the generalised Riemann hypothesis. Consequently, the study of their extreme values has attracted considerable attention.
The study of extreme values of Dirichlet L-functions can be traced back to the work of Littlewood. Granville and Soundararajan [Reference Granville and Soundararajan9] established a sharp lower bound for Dirichlet L-functions at
$s=1$
. They showed that for any
$A \ge 10$
and any sufficiently large prime q, there exist at least
$q^{1-1/A}$
characters
$\chi \pmod {q}$
such that
Here,
$\gamma $
denotes the Euler–Mascheroni constant. Subsequently, Aistleitner et al. [Reference Aistleitner, Mahatab, Munsch and Peyrot3] sharpened this result by proving that, for sufficiently large primes q, there exists a nonprincipal character
$\chi \pmod q$
such that
where
$C=1+\log \log 4 \approx 1.33$
. This is currently the best known result. They also obtained a probabilistic result concerning the characters
$\chi $
for which such extreme values occur. Moreover, for any fixed
$\sigma $
in the interval
$1/2<\sigma <1$
, they proved that there exists a nonprincipal character
$\chi \pmod q$
such that
for some constant
$C(\sigma )>0$
.
Yang [Reference Yang13] studied extreme values of derivatives of Dirichlet L-functions at
$s=1$
in depth. By combining estimates for smooth numbers with the resonance method, he proved that, for sufficiently large primes q,
uniformly for all positive integers
$\ell \le (\log \log \log q)/(\log \log \log \log q)$
. Here,
${Y_\ell = \int _0^\infty u^\ell \rho (u)\,du}$
and
$\rho (u)$
denotes the Dickman function. For studies on the extreme values of derivatives of Dirichlet L-functions and related functions, see [Reference Dong, Song, Wang and Zhang7, Reference Dong and Wei8, Reference Yang12, Reference Yang and Zhao15].
The resonance method is currently the main tool for investigating extreme values. Its basic idea originates from Voronin’s work [Reference Voronin11] in 1988. Soundararajan [Reference Soundararajan10] subsequently improved Voronin’s method and made it more concise and efficient. Further refinements were introduced by Aistleitner [Reference Aistleitner1], Bondarenko and Seip [Reference Bondarenko and Seip4, Reference Bondarenko and Seip5], and several other authors. For more details on the resonance method, see [Reference Aistleitner, Mahatab and Munsch2, Reference Chirre6, Reference Yang and Zhao14].
Inspired by Yang’s work [Reference Yang13], we study extreme values of derivatives of Dirichlet L-functions for
$1/2<\sigma <1$
. We obtain the following theorem by applying the long resonator method.
Theorem 1.1. Fix
$\ell \in \mathbb {N}$
and
$\sigma \in (1/2,1)$
. Then, there exists a constant
$c_{\sigma ,\ell }>0$
such that, for every sufficiently large prime q, one can find a nonprincipal Dirichlet character
$\chi \pmod q$
satisfying
In the case
$\ell =0$
, Theorem 1.1 coincides with (1.1). A similar result on the extreme values of derivatives of the Riemann zeta function can be found in [Reference Yang12, Theorem 2(B)] and the present work generalises that result to Dirichlet L-functions.
This paper is organised as follows. In Section 2, we introduce the resonator and establish a truncation formula for derivatives of Dirichlet L-functions. In Section 3, we apply the long resonator method to prove Theorem 1.1.
2 Preliminaries
In this section, we carry out some preliminary work. We begin with the following asymptotic formula, which shows that derivatives of Dirichlet L-functions can be effectively approximated by a truncated Dirichlet series.
Lemma 2.1. Fix
$\ell \in \mathbb {N}_+$
and
$\sigma \in (1/2,1)$
. When q is sufficiently large, for any nonprincipal character
$\chi \pmod {q}$
,
Proof. Trivially,
Using partial summation together with the Pólya–Vinogradov inequality,
Substituting this into (2.1) completes the proof of Lemma 2.1.
Next, we construct the resonator
$R(\chi )$
. Define
$Y= \eta \log q \log \log q$
, where
$0 < \eta < (2\log 4)^{-1} \sigma $
. As in [Reference Aistleitner, Mahatab, Munsch and Peyrot3], define
$r(n)$
to be a completely multiplicative function whose values at primes p are given by
Furthermore, define the resonator
Since
$r(n)$
is multiplicative,
$R(\chi )$
can be written in the Euler product form
3 Proof of Theorem 1.1
In this section, we prove Theorem 1.1 using the long resonator method. Let
$\mathcal {G}_q$
denote the set of all Dirichlet characters
$\chi $
modulo q. Since
$\chi (q)=0$
for every Dirichlet character modulo q, the term
$n=q$
in Lemma 2.1 vanishes. We therefore define
Furthermore, define the two sums
For
$S_1$
, we expand
$|R(\chi )|^2$
and apply the orthogonality of Dirichlet characters, which gives
where
$\phi (n)$
is Euler’s totient function. As
$r(1)=1$
, retaining only the term
$m=n=1$
and using the classical lower bound for Euler’s totient function, we obtain the crude lower bound
For the principal character
$\chi _0$
, it follows from the prime number theorem that
Together with
this yields
It follows from
$0 < \eta < (2\log 4)^{-1} \sigma $
that
Therefore, the contribution of the principal character
$\chi _0$
is negligible compared with the lower bound for
$S_1$
given in (3.2).
Denote by
$\mathcal {G}_q^\ast $
the set of all nonprincipal Dirichlet characters modulo q, that is,
$\mathcal {G}_q^\ast = \mathcal {G}_q \setminus \{\chi _0\}$
and define the two sums
Combining
$S_1^\ast \le S_1$
and (3.2) gives
Thus,
We now establish a lower bound for the ratio
$S_2/S_1$
. To this end, expanding
$P(\chi )$
and
$|R(\chi )|^2$
in
$S_2$
,
The orthogonality of Dirichlet characters implies that
Since all terms on the right-hand side are nonnegative, we may retain only those with
$k\mid n$
, which gives the crude lower bound
For every integer k occurring in (3.4), we have
$1\leq k<q$
. Since q is prime, it follows that
$(k,q)=1$
. Therefore,
Combining this observation with (3.1) and (3.4),
Here, the second equality follows from
$r(q)=0$
since
$Y<q$
for sufficiently large q.
If
$k> q$
, then
$k^{-\sigma } \le q^{-\sigma /2} k^{-\sigma /2}$
; hence,
The sum on the right-hand side of the above formula is bounded by
The prime number theorem gives
Thus,
The above argument shows that
Since
$Y\ge 2$
for sufficiently large q, we have
$r(2)=1/2$
. Thus,
Here, we employ the fact that
$r(n)$
is a completely multiplicative function. Combining this with (3.6), we obtain the lower bound
Set
Then, by the definition of
$r(n)$
,
Thus,
The prime number theorem shows that, when
$1/2<\sigma <1$
,
Recalling that
$Y= \eta \log q \log \log q$
,
Combining (3.3), (3.5), (3.7) and (3.8), and using Lemma 2.1, we complete the proof of Theorem 1.1.
Acknowledgements
The authors thank the referee for the valuable suggestions, which have improved the readability of this paper. The authors are grateful to Professor Zhonghua Li for the encouragement and to Dr. Zikang Dong, Dr. Qiyu Yang and Dr. Guang-liang Zhou for their helpful comments.


