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Article

Joint Approximation by the Riemann and Hurwitz Zeta-Functions in Short Intervals

by
Antanas Laurinčikas
Institute of Mathematics, Faculty of Mathematics and Informatics, Vilnius University, Naugarduko Str. 24, LT-03225 Vilnius, Lithuania
Symmetry 2024, 16(12), 1707; https://doi.org/10.3390/sym16121707
Submission received: 9 November 2024 / Revised: 12 December 2024 / Accepted: 16 December 2024 / Published: 23 December 2024
(This article belongs to the Section Mathematics)

Abstract

:
In this study, the approximation of a pair of analytic functions defined on the strip { s = σ + i t C : 1 / 2 < σ < 1 } by shifts ( ζ ( s + i τ ) , ζ ( s + i τ , α ) ) , τ R , of the Riemann and Hurwitz zeta-functions with transcendental α in the interval [ T , T + H ] with T 27 / 82 H T 1 / 2 was considered. It was proven that the set of such shifts has a positive density. The main result was an extension of the Mishou theorem proved for the interval [ 0 , T ] , and the first theorem on the joint mixed universality in short intervals. For proof, the probability approach was applied.

1. Introduction

Denote by s = σ + i t is a complex variable and 0 < α 1 is a fixed parameter. The Riemann and Hurwitz zeta-functions ζ ( s ) and ζ ( s , α ) , for σ > 1 , are defined by the Dirichlet series as follows:
ζ ( s ) = m = 1 1 m s and ζ ( s , α ) = m = 0 1 ( m + α ) s ,
The functions have analytic continuations to the whole complex plane, except for point s = 1 , which is a simple pole with residues 1. Moreover, the function ζ ( s ) , for σ > 1 , can be defined by the Euler product as follows:
ζ ( s ) = p P 1 1 p s 1 ,
where P is the set of all prime numbers.
The functions ζ ( s ) and ζ ( s , α ) are important tools for research in the analytic number theory. The function ζ ( s ) is the main tool for investigating the distribution of prime numbers in the set N , while the function ζ ( s , α ) with rational parameter α is applied for studying prime numbers in arithmetical progressions. However, the range of applications of the functions ζ ( s ) and ζ ( s , α ) is significantly wider than the distribution of primes. They are used also in function theory, algebraic number theory, functional analysis, probability theory, and even in quantum mechanics, cosmology, and music [1,2,3,4,5].
One of the most interesting applications of the functions ζ ( s ) and ζ ( s , α ) is connected to a very important problem of the function theory—the approximation of analytic functions. At present, it is known that analytic functions defined in the strip D = { s C : 1 / 2 < σ < 1 } can be approximated by shifts ζ ( s + i τ ) (the case of non-vanishing analytic functions) or by shifts ζ ( s + i τ , α ) , τ R , for some classes of the parameter α . The latter property of zeta-functions is called universality and, for the function ζ ( s ) , was proved by S. M. Voronin in [6,7]. The initial form of the Voronin universality theorem was improved by various authors (see [8,9,10,11,12,13,14]), but its remains the same in essence: the set ζ ( s + i τ ) , τ R , is dense in the space of analytic functions. For the statement of a modern version of Voronin’s theorem, the following notation is convenient. The class of compact sets of the strip D with connected complements is denoted by K , and the class of continuous functions that are analytic in the interior of K by H 0 ( K ) with K K . Moreover, let meas A stand for the Lebesgue measure of a measurable set A R , and
L T ( ) = 1 T meas { τ [ 0 , T ] : } ,
where in place of dots, a condition satisfied by τ is to be written. Then, we have the following statement [8,9,10,11,12,13,14]:
Theorem 1.
Let  K K  and  f ( s ) H 0 ( K ) Then, for every  ε > 0
lim inf T L T sup s K | f ( s ) ζ ( s + i τ ) | < ε > 0 .
Moreover, the limit 
lim T L T sup s K | f ( s ) ζ ( s + i τ ) | < ε
 exists and is positive for all but at most countably many  ε > 0 .
The problem of the approximation of analytic functions by shifts ζ ( s + i τ , α )  is more complicated and depends on the arithmetic of the parameter  α . The simplest case is of transcendental  α , i.e., when  α  is not a root of any polynomial  p ( s ) 0  with rational coefficients. In this case, the set  { log ( m + α ) : m N 0 } N 0 = N { 0 } , is linearly independent over  Q , and we have a certain analogy with the function  ζ ( s ) , where the linear independence of the set  { log p : p P }  is applied. The case of rational parameter  α = a / q ( a , q ) = 1 , in virtue of the following representation: 
ζ s , a q = q s φ ( q ) χ ( mod q ) χ ¯ ( a ) L ( s , χ ) ,
where a summing runs over all Dirichlet characters modulus q L ( s , χ )  denotes the Dirichlet L-functions, and  φ ( q )  is the Euler totient function, is reduced to the simultaneous approximation of a tuple of  φ ( q )  analytic functions by shifts  ( L ( s + i τ , χ 1 ) , , L ( s + i τ , χ φ ( q ) ) ) . More precisely, the following result by different methods was obtained in [8,9,14] (see also [12,15]). The class of continuous on K functions that are analytic in the interior of K is denoted by  H ( K )  with  K K .
Theorem 2.
Suppose that the parameter α is transcendental, or rational  1 , 1 / 2 . Let  K K  and  f ( s ) H ( K ) . Then, for every   ε > 0
lim inf T L T sup s K | f ( s ) ζ ( s + i τ , α ) | < ε > 0 .
Moreover, the limit 
lim T L T sup s K | f ( s ) ζ ( s + i τ , α ) | < ε
 exists and is positive for all but at most countably many  ε > 0 .
The cases α = 1 and α = 1 / 2 are excluded in Theorem 2 because ζ ( s , 1 ) = ζ ( s ) and
ζ s , 1 2 = 2 s 1 ζ ( s ) ,
and, for them, the statement of Theorem 1 with class H 0 ( K ) is valid.
The most complicated case is of algebraic irrational parameter α . This case was studied in [16]. The degree of α is denoted by d. Let θ = 4 ( 27 ( 4.45 ) 2 ) 1 and β = θ d 2 . Then, in [16], the following statement was proven to be true.
Theorem 3.
Suppose that the parameter α is algebraic irrational. Let γ ( 0 , β ) , 1 β + γ σ 0 1 , s 0 = σ 0 + i t 0 , and f ( s ) be continuous functions on | s s 0 | r , r > 0 and analytic in the interior of that disc. Moreover, let 0 < a < 1 and ε ( 0 , | f ( s 0 ) | ) . Then, for all but finitely many α [ a , 1 ] , of degree at most d 0 2 θ 1 / d 0 2 + γ with
d 0 θ 1 σ 0 + γ 1 / 2 ,
there exist τ [ T , 2 T ] and δ = δ ( ε , f , T ) > 0 such that
max | s s 0 | δ r | f ( s ) ζ ( s + i τ , α ) | < 3 ε ,
where T = T ( ε , f , α ) is explicitly given, the set of exceptional α is effectively described, and δ is also effectively computable.
Theorems 1–3 are devoted to the approximation of one function from a wide class of analytic functions. Also, there are the so-called joint universality theorems in which a tuple of analytic functions is approximated simultaneously by shifts of zeta-functions. The first joint universality result can also be found in Voronin [17] and deals with Dirichlet L-functions with pairwise non-equivalent characters (see also [9,18,19]). A joint universality theorem for a pair of Hurwitz zeta-functions was given in [20]. The joint approximation of analytic functions by shifts of Hurwitz zeta- functions involving imaginary parts of non-trivial zeros of the Riemann zeta-function was discussed in [21]. However, later, many joint universality theorems were obtained for functions of the same name (for more results, see [12]). For illustration purposes, we present one example. For j = 1 , , r , let 0 < α j 1 , and
L ( α 1 , , α r ) = { log ( m + α j ) : m N 0 , j = 1 , , r } .
Theorem 4.
([15]). Suppose that the set L ( α 1 , , α r ) is linearly independent over Q . For j = 1 , , r , let K j K and f j ( s ) H ( K j ) . Then, for every ε > 0 ,
lim inf T L T sup 1 j r sup s K j | f j ( s ) ζ ( s + i τ , α j ) | < ε > 0 .
Also, some problems of joint universality for Hurwitz zeta-functions can be found in [22].
In [23], H. Mishou initiated a new type of joint mixed universality theorems; he proved a joint universality theorem for two functions of different types, for the Riemann zeta-function and Hurwitz zeta-function. Here, it is important to stress that ζ ( s ) has the Euler product, while ζ ( s , α ) has no such a product for α 1 and α 1 / 2 . Moreover, the function ζ ( s ) satisfies the symmetric functional equation
ξ ( s ) = ξ ( 1 s ) , s C , ξ ( s ) = π s / 2 Γ s 2 ζ ( s ) ,
where Γ ( s ) is the Euler gamma-function, while, for ζ ( s , α ) , the following non-symmetric equations connecting s and 1 s are true:
ζ ( 1 s , α ) = Γ ( s ) ( 2 π ) s e π i s / 2 m = 1 e 2 π i m α m s + e π i s / 2 m = 1 e 2 π i m α m s , σ > 1 ,
or
ζ ( s , α ) = 2 Γ ( 1 s ) ( 2 π ) 1 s sin π s 2 m = 1 cos ( 2 π m α ) m 1 s + cos π s 2 m = 1 sin ( 2 π m α ) m 1 s , σ < 0 .
This is one of the causes of differences in the value distribution of ζ ( s ) and ζ ( s , α ) and also reflects the approximate functional equation for ζ ( s , α ) , which is the main ingredient for the proof of the mean square estimate in short intervals [24].
Theorem 5.
([23]). Suppose that the parameter α is transcendental. Let K 1 , K 2 K and f 1 ( s ) H 0 ( K 1 ) , f 2 ( s ) H ( K 2 ) . Then, for every ε > 0 ,
lim inf T L T sup s K 1 | f 1 ( s ) ζ ( s + i τ ) | < ε , sup s K 2 | f 2 ( s ) ζ ( s + i τ , α ) | < ε > 0 .
The thesis [25] is devoted to joint discrete universality for the Riemann and Hurwitz zeta-functions. Mixed joint universality is studied also for more general zeta-functions. We mention the works [26,27,28,29,30,31]. The weighted versions of the Mishou theorem are proven in [32]. Theorems 1, 2, 4, and 5 have one common shortcoming: they imply that the set of approximating shifts is infinite; however, they do not provide any algorithm to find at least one approximating shift. In this sense, these theorems are ineffective. Of course, it is difficult to discuss concrete approximation shifts; however, some additional information on the efficacy of universality theorems is always useful. In Theorem 3, the efficacy of approximation is described by indication of explicitly given interval [ T , 2 T ] containing τ such that ζ ( s + i τ , α ) is an approximating shift. This is a very good step in the effectivization direction.
In contrast to Theorem 3, the proofs of Theorems 1, 2, 4, and 5 are based on measure theory; thus, it is impossible to find an explicitly given interval containing τ with the approximation property. Therefore, there is another method to consider approximating shifts with τ in the interval of lengths shorter than T or, more precisely, o ( T ) as T . This method leads to universality theorems in short intervals. For the function ζ ( s ) , the first universality theorem of such a type was obtained in [33]. Let
L T , H ( ) = 1 H meas { τ [ T , T + H ] : } ,
where in place of dots, a condition satisfied by τ is to be written.
Theorem 6.
([33]). Suppose that T 1 / 3 ( log T ) 26 / 15 H T . Let K K , f ( s ) H 0 ( K ) . Then, for every ε > 0 ,
lim inf T L T , H sup s K | f ( s ) ζ ( s + i τ ) | < ε > 0 .
Moreover, “lim inf” can be replaced by “lim” for all but at most countably many ε > 0 .
Recently, improvements in Theorem 6 were given in [34].
An analog of Theorem 6 for the Hurwitz zeta-function is given in [35].
Theorem 7.
([35]). Suppose that T 27 / 82 H T 1 / 2 , and the parameter α is transcendental. Let K K and f ( s ) H ( K ) . Then, for every ε > 0 ,
lim inf T L T , H sup s K | f ( s ) ζ ( s + i τ , α ) | < ε > 0 .
Moreover, the lower limit can be replaced by a limit for all but at most countably many ε > 0 .
The aim of this study is to obtain a version of Theorem 5 in short intervals.
Theorem 8.
Suppose that T 27 / 82 H T 1 / 2 , and the parameter α is transcendental. Let K 1 , K 2 K and f 1 ( s ) H 0 ( K 1 ) , f 2 ( s ) H ( K 2 ) . Then, for every ε > 0 ,
lim inf T L T , H sup s K 1 | f 1 ( s ) ζ ( s + i τ ) | < ε , sup s K 2 | f 2 ( s ) ζ ( s + i τ , α ) | < ε > 0 .
Moreover, the lower limit can be replaced by a limit for all but at most countably many ε > 0 .
Using short intervals extends and improves the Mishou theorem on joint mixed universality for the functions ζ ( s ) and ζ ( s , α ) and is the novel approach presented in this article.
For effectivization aims of approximation, the quantity of H must be as small as possible. On the other hand, H is closely connected to a very important but complicated problem of analytic number theory on the mean square estimates of the functions ζ ( s ) and ζ ( s , α ) in short intervals. Unfortunately, at present, we only have a result of H T 27 / 82 in the latter problem (see Lemmas 2 and 3 below).
Mean square estimates together with a joint probabilistic limit theorem for the pair ( ζ ( s ) , ζ ( s , α ) ) in the space of analytic functions occupy a central place in the proof of Theorem 8 in short intervals for the functions ζ ( s ) and ζ ( s , α ) .

2. Mean Square Estimates

The first results for the Riemann zeta-function in short intervals were obtained by D. R. Heath-Brown, J.-M. Deshouillers, A. Ivič, H. Iwaniec, M. Jutila, A. A. Karatsuba, G. Kolesnik (for references, see [36]). We recall one mean square estimate from [36].
Lemma 1.
Let ( κ , λ ) be an exponential pair and 1 / 2 < σ < 1 fixed. Then, for T ( κ + λ + 1 2 σ ) / 2 ( κ + 1 ) × ( log T ) ( 2 + κ ) / ( κ + 1 ) H T , 1 + λ κ 2 σ , we have uniformly in H
T H T + H | ζ ( σ + i t ) | 2 d t H .
Lemma 2.
Suppose that α 1 / 2 , 1 , and 1 / 2 < σ 7 / 12 is fixed. Then, for T 27 / 82 H T , uniformly in H
T H T + H | ζ ( σ + i t ) | 2 d t σ H .
Proof.  
The lemma follows from Lemma 1 by taking the exponential pair ( 11 / 30 , 16 / 30 ) . □
Lemma 3.
Suppose that α 1 / 2 , 1 , and 1 / 2 < σ 7 / 12 is fixed. Then, for T 27 / 82 H T σ , uniformly in H
T H T + H | ζ ( σ + i t , α ) | 2 d t σ , α H .
Proof.  
The lemma is Theorem 2 from [24], where its proof is presented. □
Let θ > 1 / 2 be fixed, and, for n N ,
v n ( m ) = exp m n θ .
Define the series
ζ n ( s ) = m = 1 v n ( m ) m s
which absolutely converges in any half-plane σ > σ 0 with finite σ 0 .
Lemma 4.
Suppose that K D is a compact set and T 27 / 82 H T . Then
lim n lim sup T 1 H T T + H sup s K | ζ ( s + i τ ) ζ n ( s + i τ ) | d τ = 0 .
Proof.  
Let
l n ( s ) = 1 θ Γ s θ n s .
We use the following integral representation [10]:
ζ n ( s ) = 1 2 π i θ i θ + i ζ ( s + z ) l n ( z ) d z
which is a result of the classical Mellin formula that yields
v n ( m ) = 1 2 π i θ i θ + i 1 θ Γ s θ m n s d s .
Let K D be a fixed compact set. Then, K is closed and bounded; hence, there exists a positive number δ < 1 / 12 such that 1 / 2 + 2 δ σ 1 δ for all s = σ + i t K . We take θ = 1 / 2 + δ and θ ^ = 1 / 2 + δ σ . Then, θ ^ < 0 and θ ^ 1 / 2 + δ 1 + δ = 2 δ 1 / 2 > 1 / 2 δ = θ . The integrand in (1) has only two simple poles in the strip θ ^ < Re z < θ , i.e., a pole at the point z = 0 of the function Γ ( s / θ ) and a pole at the point z = 1 s of the function ζ ( s + z ) . Therefore, using the well-known estimate
Γ ( σ + i t ) exp { c | t | } , c > 0 ,
which is uniform in σ ( σ 1 , σ 2 ) with every σ 1 < σ 2 , and replacing θ by θ ^ in the line of integration in (1), via the residue theorem, we obtain, for s K ,
ζ n ( s ) ζ ( s ) = 1 2 π i θ ^ i θ ^ + i ζ ( s + z ) l n ( z ) d z + l n ( 1 s ) .
This gives, for s K ,
ζ n ( s ) ζ ( s ) = 1 2 π ζ σ + i t + 1 2 + δ σ + i u l n 1 2 + δ σ + i u d u + l n ( 1 s ) .
Hence, for s K ,
ζ n ( s + i τ ) ζ ( s + i τ ) ζ 1 2 + δ + i t + i τ + i u l n 1 2 + δ σ + i u d u + sup s K l n ( 1 s i τ ) ,
and, after change t + u by u, we obtain
sup s K ζ n ( s + i τ ) ζ ( s + i τ ) ζ 1 2 + δ + i τ + i u sup s K l n 1 2 + δ s + i u d u + sup s K l n ( 1 s i τ ) .
In view of (2), we have, for s K ,
l n 1 2 + δ s + i u δ n 1 / 2 + δ σ exp c θ | u t | δ , K n δ exp { c 1 | u | }
with c 1 > 0 . Moreover, it is well known that, for σ 1 / 2 ,
ζ ( σ + i t ) t 1 σ , t 2 .
This and (4) imply that
log 2 T + log 2 T ζ 1 2 + δ + i τ + i u sup s K l n 1 2 + δ s + i u d u δ , K n δ log 2 T + log 2 T ( | τ | + | u | ) 1 / 2 exp { c 1 | u | } d u δ , K n δ ( | τ | + 1 ) 1 / 2 exp { c 2 log 2 T } , c 2 > 0 .
Therefore, via (3), we find
1 H T T + H sup s K | ζ ( s + i τ ) ζ n ( s + i τ ) | d τ δ , K log 2 T log 2 T 1 H T T + H ζ 1 2 + δ + i τ + i u d τ sup s K l n 1 2 + δ s + i u d u + 1 H T T + H sup s K | l n ( 1 s i τ ) | d τ + n δ exp { c 2 log 2 T } H T T + H ( | τ | + 1 ) 1 / 2 d τ = def J 1 + J 2 + J 3 .
Using the Cauchy–Schwarz inequality gives
T T + H ζ 1 2 + δ + i τ + i u d τ T T + H ζ 1 2 + δ + i τ + i u 2 d τ 1 / 2 1 H T H | u | T + H + | u | ζ 1 2 + δ + i τ 2 d τ 1 / 2 .
For | u | log 2 T and large T,
H + | u | T 1 / 2 + log 2 T T .
Therefore, (6) and Lemma 2 show that, for | u | log 2 T ,
1 H T T + H ζ 1 2 + δ + i τ + i u d τ δ 1 H ( H + | u | ) 1 / 2 δ ( 1 + | u | ) 1 / 2 .
This and (4) give the estimate
J 1 δ , K n δ log 2 T log 2 T exp { c 1 | u | } ( 1 + | u | ) 1 / 2 d u δ , K u δ .
Similarly to (4), we obtain that, for s K ,
l n ( 1 s i τ ) n 1 σ exp { c 1 | t + τ | } K n 1 / 2 2 δ exp { c 3 | τ | } , c 3 > 0 .
Thus,
J 2 K n 1 / 2 2 δ 1 H T T + H exp { c 3 | τ | } d τ K n 1 / 2 2 δ H .
It is easily seen that
J 3 n δ exp { c 2 log 2 T } T 1 / 2 .
This, (5), (7), and (8) lead to the following estimate:
1 H T T + H sup s K | ζ ( s + i τ ) ζ n ( s + i τ ) | d τ δ , K n δ + n 1 / 2 2 δ H 1 + n δ exp { c 2 log 2 T } T 1 / 2 .
Taking T , and then n , gives the equality of the lemma. □
Recall a metric in H ( D ) , inducing its topology [37]. There exists a sequence { K l } of embedded compact sets lying in D such that
l = 1 K l = D ,
and every compact set K D lies in some set K l . Then, for g 1 , g 2 H ( D ) , denoting
ρ ( g 1 , g 2 ) = l = 1 2 l sup s K l | g 1 ( s ) g 2 ( s ) | 1 + sup s K | g 1 ( s ) g 2 ( s ) | ,
we have the metric ρ that induces the topology of H ( D ) .
The latter formula with Lemma 4 yields the following statement.
Lemma 5.
Suppose that T 27 / 82 H T . Then the equality
lim n lim sup T 1 H T T + H ρ ζ ( s + i τ ) , ζ n ( s + i τ ) d τ = 0
holds.
A similar lemma for the Hurwitz zeta-function was obtained in [35]. For the same θ as above, define
v n ( m , α ) = exp m + α n θ .
and
ζ n ( s , α ) = m = 0 v n ( m , α ) ( m + α ) s
Then, the latter series, as ζ n ( s ) , is absolutely convergent for σ > σ 0 , with arbitrary finite σ 0 .
Lemma 6.
Suppose that T 27 / 82 H T 1 / 2 , and α 1 / 2 or 1. Then
lim n lim sup T 1 H T T + H ρ ζ ( s + i τ , α ) , ζ n ( s + i τ , α ) d τ = 0 .
Proof.  
The lemma is Lemma 10 from [35], where its proof is given. □
For
g ̲ k = ( g k 1 , g k 2 ) H 2 ( D ) , k = 1 , 2 ,
set
ρ 2 ( g ̲ 1 , g ̲ 2 ) = max ρ ( g 11 , g 12 ) , ρ ( g 21 , g 22 ) .
Then ρ 2 is a metric that induces the topology of H 2 ( D ) . This definition of ρ 2 and Lemmas 5 and 6 imply the following lemma. For brevity, let
ζ ̲ ( s , α ) = ζ ( s ) , ζ ( s , α )
and
ζ ̲ n ( s , α ) = ζ n ( s ) , ζ n ( s , α ) .
Lemma 7.
Suppose that  T 27 / 82 H T 1 / 2 , and  α 1 / 2  or 1. Then
lim n lim sup T 1 H T T + H ρ 2 ζ ̲ ( s + i τ , α ) , ζ ̲ n ( s + i τ , α ) d τ = 0 .

3. Limit Theorem

In this section, we will consider the weak convergence for
P T , H , α ( A ) = L T , H ζ ̲ ( s + i τ , α ) A , A B ( H 2 ( D ) ) ,
as T , with H restricted in Lemma 7, and B ( X ) denotes the Borel σ -field of the space X .
We start with the weak convergence of probability measures on a certain topological group. Let
Ω 1 = p P { s C : | s | = 1 } , Ω 2 = m N 0 { s C : | s | = 1 } , and Ω = Ω 1 × Ω 2 .
Since Ω 1 and Ω 2 with the product topology and pointwise multiplication are compact topological groups, the Tikhonov theorem implies that Ω is again a compact topological group. Thus, on ( Ω 1 , B ( Ω 1 ) ) , ( Ω 2 , B ( Ω 2 ) ) , and ( Ω , B ( Ω ) ) , the probability Haar measures m 1 H , m 2 H , and m H , respectively, can be defined. We notice that m H = m 1 H × m 2 H , i. e., if A = A 1 × A 2 , A 1 B ( Ω 1 ) , A 2 B ( Ω 2 ) , then
m H ( A ) = m 1 H ( A 1 ) m 2 H ( A 2 ) .
For ω Ω , we have ω = ( ω 1 , ω 2 ) with ω 1 = ( ω 1 ( p ) : p P ) and ω 2 = ( ω 2 ( m ) : m N 0 ) .
For A B ( Ω ) , set
P T , H , α Ω ( A ) = L T , H p i τ : p P , ( m + α ) i τ : m N 0 A .
Lemma 8.
Suppose that T 27 / 82 H T 1 / 2 , and α is transcendental. Then, P T , H , α Ω converges weakly to the Haar measure m H as T .
Proof.  
We use similar arguments as in the case τ [ 0 , T ] . Let F T , H , α ( k ̲ 1 , k ̲ 2 ) , k ̲ 1 = ( k 1 p : k 1 p Z , p P ) , k ̲ 2 = ( k 2 m : k 2 m Z , m N 0 ) , be the Fourier transform of P T , H , α Ω , i. e.,
F T , H , α ( k ̲ 1 , k ̲ 2 ) = Ω * p P ω k 1 p ( p ) * m N 0 ω k 2 m ( m ) d P T , H , α Ω ,
where the star ∗ shows that only a finite number of integers k 1 p and k 2 m are not zeroes. Thus, taking into account the definition of the measure P T , H , α Ω , we have
F T , H , α ( k ̲ 1 , k ̲ 2 ) = 1 H T T + H * p P p i τ k 1 p * m N 0 ( m + α ) i τ k 2 m d τ = 1 H T T + H exp i τ * p P k 1 p log p + * m N 0 k 2 m log ( m + α ) d τ .
We have to show that
lim T F T , H , α ( k ̲ 1 , k ̲ 2 ) = 1 if ( k ̲ 1 , k ̲ 2 ) = ( 0 ̲ , 0 ̲ ) , 0 if ( k ̲ 1 , k ̲ 2 ) ( 0 ̲ , 0 ̲ ) ,
where 0 ̲ = ( 0 , 0 , ) . Obviously, by (9),
F T , H , α ( 0 ̲ , 0 ̲ ) = 1 .
Therefore, only the case ( k ̲ 1 , k ̲ 2 ) ( 0 ̲ , 0 ̲ ) remains for consideration. Since α is transcendental, the set L ( α ) = { log ( m + α ) : m N 0 } is linearly independent over Q . The set { log p : p P } is also linearly independent over Q . The linear independence over Q for the set L ( P , α ) = def { ( log p : p P ) , ( log ( m + α ) : m N 0 ) } is easily seen. Actually, if, for some non-zeroes k 1 p 1 , , k 1 p r , k 2 m 1 , , k 2 m v ,
k 1 p 1 log p 1 + k 1 p r log p r + k 2 m 1 log ( m 1 + α ) + k 2 m v log ( m v + α ) = 0 ,
then
( m 1 + α ) k 21 ( m v + α ) k 2 v = p 1 k 11 p r k 1 r .
From this, it follows that there exists a polynomial p ( s ) with rational coefficients such that p ( α ) = 0 , and this contradicts the transcendence of α .
The linear independence of the set L ( P , α ) shows that, in the case ( k ̲ 1 , k ̲ 2 ) ( 0 ̲ , 0 ̲ ) ,
A ( k ̲ 1 , k ̲ 2 ) = def * p P k 1 p log p + * m N 0 k 2 m log ( m + α ) 0 .
Hence, in view of (9),
F T , H , α ( k ̲ 1 , k ̲ 2 ) = exp { i T A ( k ̲ 1 , k ̲ 2 ) } exp { i ( T + H ) A ( k ̲ 1 , k ̲ 2 ) } i H A ( k ̲ 1 , k ̲ 2 ) .
Thus, for ( k ̲ 1 , k ̲ 2 ) ( 0 ̲ , 0 ̲ ) ,
lim T F T , H , α ( k ̲ 1 , k ̲ 2 ) = 0 ,
and with (11), we obtain (10). The lemma is proven to be true. □
Now, we are in position to consider the weak convergence for
P T , H , n , α ( A ) = def L T , H ζ ̲ n ( s + i τ , α ) A , A B ( H 2 ( D ) ) .
For this, define u n , α : Ω H 2 ( D ) by
u n , α ( ω ) = ζ ̲ n ( s , ω , α ) , ω Ω ,
where
ζ ̲ n ( s , ω , α ) = ζ n ( s , ω 1 ) , ζ n ( s , ω 2 , α ) ,
ζ n ( s , ω 1 ) = m = 1 ω 1 ( m ) , v n ( m ) m s , ω 1 ( m ) = p l m p l + 1 m ω 1 l ( p ) ,
and
ζ n ( s , ω 2 , α ) = m = 0 ω 2 ( m ) v n ( m , α ) ( m + α ) s .
Since the series for ζ n ( s , ω 1 ) and ζ n ( s , ω 2 , α ) are absolutely convergent in every half-plane σ > σ 0 , the mapping u n , α is continuous; hence, ( B ( Ω ) , B ( H 2 ( D ) ) ) -measurable. Therefore, the measure m H defines, on ( H 2 ( D ) , B ( H 2 ( D ) ) ) , the probability measure m H u n , α 1 by
m H u n , α 1 ( A ) = m H ( u n , α 1 A ) , A B ( H 2 ( D ) ) .
For brevity, let U n , α = m H u n , α 1 .
Lemma 9.
Suppose that T 27 / 82 H T 1 / 2 , and α is transcendental. Then, P T , H , n , α converges weakly to U n , α as T .
Proof.  
The definition of u n , α yields
u n , α p i τ : p P , ( m + α ) i τ : m N 0 = ζ ̲ n ( s + i τ , α ) .
Therefore, by the definitions of P T , H , α Ω and P T , H , n , α , we have
P T , H , n , α ( A ) = L T , H p i τ : p P , ( m + α ) i τ : m N 0 u n , α 1 A
for all A B ( H 2 ( D ) ) . Hence,
P T , H , n , α = P T , H , α Ω u n , α 1 .
This, the continuity of u n , α , Lemma 8, and Theorem 5.1 of [38] prove that P T , H , n , α converges weakly to U n , α . □
On ( Ω , B ( Ω ) , m H ) , define the H 2 ( D ) -valued random element ζ ̲ ( s , ω , α ) by
ζ ̲ ( s , ω , α ) = ζ ( s , ω 1 ) , ζ ( s , ω 2 , α ) ,
where
ζ ( s , ω 1 ) = m = 1 ω 1 ( m ) m s and ζ ( s , ω 2 , α ) = m = 0 ω 2 ( m ) ( m + α ) s .
We observe that the latter series are uniformly convergent on compact subsets of strip D for almost all ω 1 and ω 2 , respectively (see, for example, [10,15]). Let P ζ ̲ , α be the distribution of the random element ζ ̲ ( s , ω , α ) , i. e.,
P ζ ̲ , α ( A ) = m H ω Ω : ζ ̲ ( s , ω , α ) A , A B ( H 2 ( D ) ) .
In [23], for the proof of Theorem 5, a limit theorem for the functions ζ ( s ) and ζ ( s , α ) with transcendental α was obtained. For A B ( H 2 ( D ) ) , let
P T , α ( A ) = L T ζ ̲ ( s + i τ , α ) A .
Then, in [23], it was proved that P T , α , as T , and U n , α , as n converges weakly to the same probability measure on ( H 2 ( D ) , B ( H 2 ( D ) ) ) , and this measure is P ζ ̲ , α . Thus, we have the following statement.
Lemma 10.
Suppose that α is transcendental. Then, U n , α converges weakly to P ζ ̲ , α as n .
Now, we are ready to prove a limit theorem for P T , H , α .
Theorem 9.
Suppose that T 27 / 82 H T 1 / 2 , and α is transcendental. Then P T , H , α converges weakly to P ζ ̲ , α as T .
Proof.  
Introduce a random variable ξ T , H defined on a certain probability space ( Ω ^ , A , μ ) and uniformly distributed on [ T , T + H ] . Define the H 2 ( D ) -valued random elements as follows:
ζ ̲ T , H , n , α = ζ ̲ T , H , n , α ( s ) = ζ n ( s + i ξ T , H ) , ζ n ( s + i ξ T , H , α )
and
ζ ̲ T , H , α = ζ ̲ T , H , α ( s ) = ζ ( s + i ξ T , H ) , ζ ( s + i ξ T , H , α ) .
Moreover, let ζ ̲ n , α denote the H 2 ( D ) -valued random element with distribution U n , α . Further on, we will use the language of convergence in distribution ( D ), i. e., we say that a random element η n , as n , converges in distribution to η if the distribution of η n , as n , converges weakly to that of η .
In virtue of Lemma 10, we have
ζ ̲ T , H , n , α T D ζ ̲ n , α .
By Lemma 10,
ζ ̲ n , α n D ζ ̲ ( s , α ) .
The definitions of ζ ̲ T , H , n , α , ζ ̲ T , H , α , and ξ T , H show that, for every ε > 0 ,
lim n lim sup T μ ρ 2 ζ ̲ T , H , α , ζ ̲ T , H , n , α ε = lim n lim sup T L T , H ρ 2 ζ ̲ ( s + i τ , α ) , ζ ̲ n ( s + i τ , α ) ε lim n lim sup T 1 ε H T T + H ρ 2 ζ ̲ ( s + i τ , α ) , ζ ̲ n ( s + i τ , α ) d τ .
Therefore, Lemma 7 implies that
lim n lim sup T μ ρ 2 ζ ̲ T , H , α , ζ ̲ T , H , n , α ε = 0 .
This equality and relations (12) and (13) show that all hypotheses of Theorem 4.2 of [38] are fulfilled because the space H 2 ( D ) is separable. In consequence,
ζ ̲ T , H , α T D ζ ̲ ( s , α ) ,
and this relation is equivalent to the weak convergence of P T , H , α to P ζ ̲ , α as T . □

4. Proof of the Main Theorem

Theorem 9 is the main ingredient of the proof of Theorem 8. However, the support of the limit measure P ζ ̲ , α is also needed. We recall that the support of P ζ ̲ , α is a minimal closed set S ζ ̲ , α H 2 ( D ) such that P ζ ̲ , α ( S ζ ̲ , α ) = 1 . The elements of S ζ ̲ , α have a property that, for every open neighborhood G of g ̲ , the inequality P ζ ̲ , α ( G ) > 0 is satisfied.
Since the space H 2 ( D ) is separable, we have [38]
B ( H 2 ( D ) ) = B ( H ( D ) ) × B ( H ( D ) ) .
Therefore, it suffices to deal with sets of the form
A = A 1 × A 2 , A 1 , A 2 B ( H ( D ) ) .
It is well known [10] that
L T ζ ( s + i τ ) A , A B ( H ( D ) ) ,
converges weakly to the measure P ζ as T , where P ζ is the distribution of the random element ζ ( s , ω 1 ) .
L T ζ ( s + i τ , α ) A , A B ( H ( D ) ) ,
with transcendental α converges weakly to the measure P ζ , α as T , where P ζ , α is the distribution of the random element ζ ( s , ω 2 , α )  [15]. Moreover, the support of P ζ is the set
S = def g H ( D ) : g ( s ) 0 or g ( s ) 0 ,
while the support of P ζ , α is the whole H ( D ) [10,15].
Lemma 11.
The support of the measure P ζ ̲ , α is the set S × H ( D ) .
Proof.  
By a property of the Haar measures m 1 H , m 2 H , and m H , and the above remark, we have
m H ( S × H ( D ) ) = m 1 H ( S ) · m 2 H ( H ( D ) ) .
This and the minimality of the sets S and H ( D ) such that m 1 H ( S ) = 1 and m 2 H ( H ( D ) ) = 1 show that S × H ( D ) is a minimal set satisfying m H ( S × H ( D ) ) = 1 . □
Proof of Theorem 8.  
By the Mergelyan theorem on the approximation of analytic functions by polynomials [39] (see also [40]), we have the existence of polynomials p ( s ) and q ( s ) such that
sup s K 1 f 1 ( s ) e p ( s ) < ε 2
and
sup s K 2 f 2 ( s ) q ( s ) < ε 2 .
We stress that the Mergelyan theorem can be applied because K 1 , K 2 K .
Define the set
G ε = ( g 1 , g 2 ) H 2 ( D ) : sup s K 1 g 1 ( s ) e p ( s ) < ε 2 , sup s K 2 g 2 ( s ) q ( s ) < ε 2 .
Then, G ε is an open neighborhood of an element ( e p ( s ) , q ( s ) ) S × H ( D ) . By Lemma 11 and properties of the support, we have
P ζ ̲ , α ( G ε ) > 0 .
Let
G ε = ( g 1 , g 2 ) H 2 ( D ) : sup s K 1 | g 1 ( s ) f 1 ( s ) | < ε , sup s K 2 | g 2 ( s ) f 2 ( s ) | < ε .
The inequalities (14)–(15) imply the inclusion of G ε G ε . Therefore, in view of (16),
P ζ ̲ , α ( G ε ) > 0 .
The set G ε is open in H 2 ( D ) . Therefore, Theorem 9 with the equivalent of weak convergence in terms of open sets (see Theorem 2.1 of [38]) gives
lim inf T P T , H , α ( G ε ) P ζ ̲ , α ( G ε ) > 0 .
This and the definitions of G ε and P T , H , α imply the first assertion of the theorem.
The boundary of the set G ε is denoted by 𝜕 G ε . Then, we have that 𝜕 G ε 1 𝜕 G ε 2 = for different positives ε 1 and ε 2 . The set G ε is a continuity set of P ζ ̲ , α if P ζ ̲ , α ( 𝜕 G ε ) = 0 . From the above remark, it follows P ζ ̲ , α ( 𝜕 G ε ) 0 for at most countably many ε > 0 . Applying Theorem 9 again in terms of continuity sets (see Theorem 2.1 of [38]), we obtain that
lim T P T , H , α ( G ε ) = P ζ ̲ , α ( G ε ) > 0
for all but at most countably many ε > 0 . This proves the second statement of the theorem. □

5. Conclusions

Let ζ ( s ) and ζ ( s , α ) denote the Riemann and Hurwitz zeta-functions, respectively, and the parameter α is transcendental. We obtained the set of shifts ( ζ ( s + i τ ) , ζ ( s + i τ , α ) ) , τ R , that approximate a given pair of analytic functions defined on the strip D = { s C : 1 / 2 < σ < 1 } , has a positive lower density in the interval [ T , T + H ] , T . Here, T 27 / 82 H T 1 / 2 . More precisely, the following result is proven. Let K 1 and K 2 be compact subsets of the strip D with connected complements, and f 1 ( s ) 0 and f 2 ( s ) continuous functions on K 1 and K 2 that are analytic inside of K 1 and K 2 , respectively. Then, for every ε > 0 ,
lim inf T 1 H meas { τ [ T , T + H ] : sup s K 1 | f 1 ( s ) ζ ( s + i τ ) | < ε sup s K 2 | f 2 ( s ) ζ ( s + i τ , α ) | < ε } > 0 .
Moreover, except for at most countably many values of ε > 0 , “lim inf” can be replaced by “lim”. This result extends that of H. Mishou [23].
We are planing to consider similar problems for discrete shifts and generalized shifts ( ζ ( s + i φ ( τ ) ) , ζ ( s + i φ ( τ ) , α ) ) with a certain function φ ( τ ) .

Funding

This research received no external funding.

Institutional Review Board Statement

Not applicable.

Informed Consent Statement

Not applicable.

Data Availability Statement

Data are contained within the article.

Acknowledgments

The author thanks the referees for their useful remarks and comments.

Conflicts of Interest

The author declare no conflicts of interest.

References

  1. Aref’eva, I.Y.; Volovich, I.V. Quantization of the Riemann zeta-function and cosmology. Int. J. Geom. Meth. Mod. Phys. 2007, 4, 881–895. [Google Scholar] [CrossRef]
  2. Elizalde, E. Zeta-functions: Formulas and applications. J. Comput. Appl. Math. 2000, 118, 125–142. [Google Scholar] [CrossRef]
  3. Elizalde, E. Zeta-functions and the cosmos—A basic brief review. Universe 2021, 7, 5. [Google Scholar] [CrossRef]
  4. Gutzwiller, M.C. Stochastic behavior in quantum scattering. Phys. D Nonlinear Phenom. 1983, 7, 341–355. [Google Scholar] [CrossRef]
  5. Maino, G. Prime numbers, atomic nuclei, symmetries and superconductivity. In Symmetries and Order: Algebraic Methods in Many Body Sytems: A Symposium in Celebration of the Career of Professor Francesco Iachello, Connecticut, USA, 5–6 October 2018; AIP Conference Proceedings; AIP Publishing LLC: Melville, NY, USA, 2019; Volume 2150, p. 030009. [Google Scholar]
  6. Voronin, S.M. Theorem on the “universality” of the Riemann zeta-function. Math. USSR Izv. 1975, 9, 443–453. [Google Scholar] [CrossRef]
  7. Voronin, S.M. Analytic Properties of Arithmetic Objects. Doctoral Thesis, V.A. Steklov Mathematical Institute, Moscow, Russia, 1977. [Google Scholar]
  8. Gonek, S.M. Analytic Properties of Zeta and L-Functions. Ph.D. Thesis, University of Michigan, Ann Arbor, MI, USA, 1979. [Google Scholar]
  9. Bagchi, B. The Statistical Behaviour and Universality Properties of the Riemann Zeta-Function and Other Allied Dirichlet Series. Ph.D. Thesis, Indian Statistical Institute, Calcutta, India, 1981. [Google Scholar]
  10. Laurinčikas, A. Limit Theorems for the Riemann Zeta-Function; Kluwer Academic Publishers: Dordrecht, The Netherlands; Boston, MA, USA; London, UK, 1996. [Google Scholar]
  11. Steuding, J. Value-Distribution of L-Functions; Lecture Notes in Mathematics; Springer: Berlin/Heidelberg, Germany; New York, NY, USA, 2007; Volume 1877. [Google Scholar]
  12. Matsumoto, K. A survey on the theory of universality for zeta and L-functions. In Number Theory: Plowing and Starring Through High Wave Forms, Proceedings of the 7th China-Japan Seminar, Fukuoka, Japan, 28 October–1 November 2013; Kaneko, M., Kanemitsu, S., Liu, J., Eds.; Series on Number Theory and Its Applications; World Scientific Publishing Co.: Hackensack, NJ, USA; London, UK; Singapore; Bejing/Shanghai/Hong Kong, China; Taipei, Taiwan; Chennai, India, 2015; pp. 95–144. [Google Scholar]
  13. Mauclaire, J.-L. Universality of the Riemann zeta function: Two remarks. Ann. Univ. Sci. Budap. Rolando Eötvös Sect. Comput. 2013, 39, 311–319. [Google Scholar]
  14. Meška, L. Modified Universality Theorems for the Riemann and Hurwitz Zeta-Functions. Ph.D. Thesis, Vilnius University, Vilnius, Lithuania, 2017. [Google Scholar]
  15. Laurinčikas, A. The joint universality of Hurwitz zeta-functions. Šiauliai Math. Semin. 2008, 3, 169–187. [Google Scholar] [CrossRef]
  16. Sourmelidis, A.; Steuding, J. On the value distribution of Hurwitz zeta-function with algebraic irrational parameter. Constr. Approx. 2022, 55, 829–860. [Google Scholar] [CrossRef]
  17. Voronin, S.M. On the functional independence of Dirichlet L-functions. Acta Arith. 1975, 27, 443–453. (In Russian) [Google Scholar]
  18. Karatsuba, A.A.; Voronin, S.M. The Riemann Zeta-Function; Walter de Gruiter: Berlin, Germany; New York, NY, USA, 1992. [Google Scholar]
  19. Bagchi, B. Joint universality theorem for Dirichlet L-functions. Math. Z. 1982, 181, 319–334. [Google Scholar] [CrossRef]
  20. Mishou, H. The joint universality theorem for a pair of Hurwitz zeta-functions. J. Number Theory 2011, 131, 2352–2367. [Google Scholar] [CrossRef]
  21. Macaitienė, R.; Šiaučiūnas, D. Joint universality of Hurwitz zeta-functions and nontrivial zeros of the Riemann zeta-function. II. Lith. Math. J. 2021, 61, 187–198. [Google Scholar] [CrossRef]
  22. Nakamura, T. The existence and the non-existence of joint t-universality for Lerch zeta-functions. J. Number Theory 2007, 125, 424–441. [Google Scholar] [CrossRef]
  23. Mishou, H. The joint value-distribution of the Riemann zeta function and Hurwitz zeta functions. Lith. Math. J. 2007, 47, 32–47. [Google Scholar] [CrossRef]
  24. Laurinčikas, A.; Šiaučiūnas, D. The mean square of the Hurwitz zeta-function in short intervals. Axioms 2024, 13, 510. [Google Scholar] [CrossRef]
  25. Atstopienė, J. Discrete Universality Theorems for the Riemann and Hurwitz Zeta-Functions. Ph.D. Thesis, Vilnius University, Vilnius, Lithuania, 2015. [Google Scholar]
  26. Genys, J.; Račkauskienė, S.; Macaitienė, R.; Šiaučiūnas, D. A mixed joint universality theorem for zeta-functions. Math. Model. Anal. 2010, 15, 431–446. [Google Scholar] [CrossRef]
  27. Pocevičienė, V.; Šiaučiūnas, D. A mixed joint universality theorem for zeta functions. II. Math. Model. Anal. 2014, 19, 52–65. [Google Scholar] [CrossRef]
  28. Kačinskaitė, R.; Matsumoto, K. The mixed joint universality for a class of zeta-functions. Math. Nachrichten 2015, 288, 1900–1909. [Google Scholar] [CrossRef]
  29. Janulis, K. Mixed Joint Universality for Dirichlet L-Functions and Hurwitz Zeta-Functions. Ph.D. Thesis, Vilnius University, Vilnius, Lithuania, 2015. [Google Scholar]
  30. Kačinskaitė, R.; Matsumoto, K. Remarks on the mixed joint universality for a class of zeta-functions. Bull. Aust. Math. Soc. 2017, 95, 187–198. [Google Scholar] [CrossRef]
  31. Balčiūnas, A.; Jasas, M.; Macaitienė, R.; Šiaučiūnas, D. On the Mishou theorem for zeta-functions with periodic coefficients. Mathematics 2023, 11, 2042. [Google Scholar] [CrossRef]
  32. Vadeikis, G. Weighted Universality Theorems for the Remann and Hurwitz Zeta-Functions. Ph.D. Thesis, Vilnius University, Vilnius, Lithuania, 2021. [Google Scholar]
  33. Laurinčikas, A. Universality of the Riemann zeta-function in short intervals. J. Number Theory 2019, 204, 279–295. [Google Scholar] [CrossRef]
  34. Andersson, J.; Garunkštis, R.; Kačinskaitė, R.; Nakai, K.; Pańkowski, Ł.; Sourmelidis, A.; Steuding, R.; Steuding, J.; Wananiyakul, S. Notes on universality in short intervals and exponential shifts. Lith. Math. J. 2024, 64, 125–137. [Google Scholar] [CrossRef]
  35. Laurinčikas, A. Universality of the Hurwitz zeta-function in short intervals. Bol. Soc. Mat. Mex. 2025, 31, 17. [Google Scholar] [CrossRef]
  36. Ivič, A. The Riemann Zeta-Function: The Theory of the Riemann Zeta-Function with Applications; John Wiley & Sons: New York, NY, USA, 1985. [Google Scholar]
  37. Conway, J.B. Functions of One Complex Variable; Springer: New York, NY, USA, 1973. [Google Scholar]
  38. Billingsley, P. Convergence of Probability Measures, 2nd ed.; John Wiley & Sons: New York, NY, USA, 1999. [Google Scholar]
  39. Mergelyan, S.N. Uniform Approximations to Functions of a Complex Variable; American Mathematical Society Translations, No. 101; American Mathematical Society: Providence, RI, USA, 1954. [Google Scholar]
  40. Walsh, J.L. Interpolation and Approximation by Rational Functions in the Complex Domain; American Mathematical Society Colloquium Publications; American Mathematical Society: Providence, RI, USA, 1960; Volume 20. [Google Scholar]
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Laurinčikas, A. Joint Approximation by the Riemann and Hurwitz Zeta-Functions in Short Intervals. Symmetry 2024, 16, 1707. https://doi.org/10.3390/sym16121707

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Laurinčikas A. Joint Approximation by the Riemann and Hurwitz Zeta-Functions in Short Intervals. Symmetry. 2024; 16(12):1707. https://doi.org/10.3390/sym16121707

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Laurinčikas, Antanas. 2024. "Joint Approximation by the Riemann and Hurwitz Zeta-Functions in Short Intervals" Symmetry 16, no. 12: 1707. https://doi.org/10.3390/sym16121707

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Laurinčikas, A. (2024). Joint Approximation by the Riemann and Hurwitz Zeta-Functions in Short Intervals. Symmetry, 16(12), 1707. https://doi.org/10.3390/sym16121707

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