Abstract
The main purpose of this paper is to use the multiple twisted Bernoulli polynomials and their interpolation functions to construct multiple twisted Dedekind type sums. We investigate some properties of these sums. By use of the properties of multiple twisted zeta functions and the Bernoulli functions involving the Bernoulli polynomials, we derive reciprocity laws of these sums. Further developments and observations on these new Dedekind type sums are given.
| Contents | |
| 1. Introduction | 1 |
| 2. Twisted Barnes’ Type (h,q)-Zeta Functions | 9 |
| 3. Twisted (h,q)-Dedekind Type Sums | 13 |
| References | 19 |
1. Introduction
Throughout this paper, we use the following notations:
- denotes the ring of integers;
- ;
- ;
- for , we denote
- is an r-th root of 1 with .
The purpose of this paper is not only to study the different types of higher-order twisted -Bernoulli numbers and polynomials, which generalize those of [1], but also to study the relations between these numbers, polynomials, and Dedekind type sums and related areas.
The main motivation is the study of a q-analogue of the generalized Barnes’ multiple zeta function (i.e., q-Barnes’ multiple zeta function in twisted version) and to introduce a new type of Dedekind sum. We prove a Dedekind’s type reciprocity law for these new sums. Our resulting generalized reciprocity formulas recover the results of Apostol [2] and Ota [3].
Many mathematicians have studied the so-called twisted Bernoulli numbers and polynomials and their interpolation functions. For more details, one can see Cenkci et al. [4], Hu-Min Soo [5], Bayad [6], Kim [7], Koblitz [8], and Simsek [9].
Let and , we assume that . By using p-adic q-integral theory, Simsek [9] defined the generating function of the twisted -Bernoulli numbers using the following generating function:
From the above equation, we have
where denotes the Kronecker symbol and the usual convention of symbolically replacing by (cf. [9,10,11,12]). The link between the twisted -extension of Bernoulli numbers and Frobenius–Euler numbers is given in [11] by the relation
where denotes the Frobenius–Euler numbers, which are defined as follows.
For with , the Frobenius–Euler numbers are defined by using of the following generating function:
are rational fractions of polynomials and were studied in great detail by Frobenius [13], who was particularly interested in their relationship to Bernoulli numbers [14] and relation (2.7) in [15].
One can observe that for , (cf. [16]) and are the Bernoulli numbers (cf. [2,3,4,5,6,7,8,9,10,11,12,13,14,15,16,17,18,19,20,21,22,23,24,25,26,27,28,29,30,31,32]).
The twisted -Bernoulli polynomials are defined in [9] by using the generating function
We easily see that . From (2), we have
The twisted -Bernoulli numbers and polynomials of order v are given in [1,10,12]) by their generating functions:
and
where .
By using (4), we obtain
Substituting (4), we see that
From the above, we arrive at the equality
From [10,12], we quote the distribution formula.
Theorem 1.
[Distribution relation]. Let v, n, . We have
where ,
It is well-known that the distribution relation is useful for the construction of distribution on the ring of p-adic integers . For more details, see [8], Chap. II. On the other hand, the above Theorem 1 and the results of Chapter II of Koblitz’s book [8] illustrate that the twisted -Bernoulli polynomials are p-adic in essence and have profound connections with the special values of certain zeta functions.
In our paper, we will construct these zeta functions, and their study will be further detailed in Section 2 and Section 3.
Let us now specify the definition of the twisted -Bernoulli numbers of order v by using the following generating function:
where and (cf. [10,12]).
By using (1) and (6), we are now ready to give the relation between the numbers and as follows. From (6), we obtain
By substituting (1) into the above, we find that
By substituting into (7), we have
Setting and in (7), we have
By using the Cauchy product in the above, we obtain
where and if .
By (6), using geometric series, we find that
For , Relation (6) is reduced to
where .
Without loss of generality and also for the simplicity of the calculations, in this section, we treat in detail only the case where . Here, our method can be extended to the general case.
After some calculations, we obtain
From the above, we find that
is equal to
Thus, we have
By using (4), we have
By identifying the coefficients of in the above formula, we obtain the q-Raabe multiplication formula for the polynomials .
Proposition 1
([10,12]). Let , v, , with and with . Then, we have
We can rewrite , defined in (9), as follows:
Now, we give some identities related to our twisted Bernoulli polynomials of higher order.
Let
where . By the well-known identity
we obtain
From the above, we have
By comparing the coefficients of on both sides of the above, we arrive at the following result.
Proposition 2.
Let , v, , with and with . Then, we have
where .
Remark 1.
We give some particular cases with .
- Taking , by Proposition 2, we obtain
- In addition, if in the above, we deduce the well-known Carlitz’s multiplication formula [17]:
- If in Proposition 2, then the Raabe formula for the usual Bernoulli polynomials is given by
- In [23], Kim investigated several properties of symmetry for the p-adic invariant integral on . By using symmetry for the p-adic invariant integral on , Kim proved (12). If and , , then we arrive at Luo’s formula [26]:
By using (12), we obtain
From the above, we obtain
Thus, we arrive at the following result.
Corollary 1.
Let v, , with and with . We have
where .
For , , from Corollary 1, we obtain
(cf. [9]).
Corollary 2.
Let , with and with . Then, we have the reduction formula
where and ; holds true between the twisted -Bernoulli polynomials and the twisted -Bernoulli numbers of order .
Proof.
By using (10), we have
here, we use the Cauchy product. By comparing the coefficients of on both sides of the above equation, we then arrive at the desired result. □
2. Twisted Barnes’ Type -Zeta Functions
In this section, we construct interpolation functions of the twisted -Bernoulli polynomials and numbers of higher order. We also give some interesting identities related to these functions. Throughout this section, we study the complex s-plane. Let with and ( is an rth root of 1) .
Note that the numbers are related to the so-called Apostol-Bernoulli numbers [26,27] and twisted Bernoulli numbers.
We decompose (2) as follows:
From the above and the relation (13), we find that
Let us define
observe that .
For , by applying the Mellin transformation to the above equation, we obtain
it is easy to see that the series converge for whole complex plane, because and .
We easily see that
Observe that for , we have
which denotes the Riemann zeta function.
The function interpolates the polynomials at negative integers as follows:
We easily see from the above that
We now construct higher-order interpolation functions.
Hence, from the above, we define the zeta functions .
Definition 1.
Let with and with . We define
where and .
In [20], the authors gave another kind of the twisted Barnes zeta function.
From (19), we find that
From the above, we arrive at the following main theorem.
Theorem 2.
[Explicit formula]. Let , with , , and with . Then, we have
where
We now give some special values of the function as follows:
Corollary 3.
Let . Then, we have
(i) Difference equation of the function :
(ii) Distribution relation of the function :
(iii) For real number y,
where
We note that it is easy to prove Corollary 3 from the definition .
Remark 2.
We give comments on some special cases.
- If , then Theorem 2 reduces towhere
- In [29], Simsek defined and studied the -Hurwitz zeta function which is related to the function :
- In addition, if , then is reduced to (cf. [16]).
- If , and , then Theorem 2 reduces to the twisted zeta functions which interpolate the twisted Bernoulli numbers:where , .
- The Lerch transcendent (cf. e.g., [32] p. 121, [21]) is the analytic continuation of the seriesThe above series converges for (, when ; when ), whereHence, the function is related to as follows:
By substituting into (19) and using Cauchy’s residue theorem for the Hankel contour, we obtain the following theorem:
Theorem 3.
[Values at negative integers]. Let and . Then, we have
From the above theorem, we arrive at the following corollary:
Corollary 4.
Let . Thus, we have
By substituting into Theorem 2, we have
Thus, we find that
3. Twisted -Dedekind Type Sums
In this section, we define twisted -Dedekind type sums. We state and prove their reciprocity law. For more details on the elliptic analogue for the Dedekind reciprocity laws, see [6].
Let us recall the Apostol–Dedekind sums :
where h and k are coprime integers with , n is a positive integer, and is the nth Bernoulli function, which is defined as follows:
and
where is the Bernoulli polynomial.
For even values of n, the sums are relatively uninteresting. However, for odd values of n, these sums have a reciprocity law, first proved by Apostol [2]:
where . If , then the Apostol–Dedekind sums reduce to the classical Dedekind sums.
We are ready to define the -twisted Dedekind sums.
Definition 2.
Let h and k be coprime integers with . Then, we define
where is an integer number and
where is defined in (14).
Example 1.
By using the well-known alternating sums of powers of consecutive -integers for ,
(cf. [10]), we then obtain the following Theorem.
Theorem 4.
[Explicit evaluation for ]. Let m and k be positive integers. Then, we have
In [3], Ota showed how to prove Apostol’s reciprocity law by using values at non-positive integers of Barnes’ double zeta function. In this section, we give a generalization of Apostol’s reciprocity law.
By substituting and into (21), and by using a method similar to that in, then we have
Setting and , where , and m, ) in the above,
where means that the above sum take pairs on non-negative integers with the exception of when . Putting in the above, we then obtain
After some elementary calculations in the above, we easily see that
By using the above, we arrive at the following theorem.
Theorem 5.
By using Theorem 5, we prove the reciprocity law of the -twisted Dedekind sums in the next theorem.
Theorem 6.
[Reciprocity law]. Let h and k be coprime integers with . Let . Then, we have
where is defined in (8).
Proof.
Remark 3.
We point out how we recover, from our Theorem 6, some known results.
- By substituting and into Theorem 6, we obtain the result of Ota ([3], [p. 8, Theorem B]):Consequently, Theorem 6 is a generalization of Ota’s theorem ([3], [p. 8, Theorem B]).
- By substituting and , into Theorem 6, then we easily arrive at (27). Thus, Theorem 6 is also a generalization of Apostol’s reciprocity theorem [2] for odd n.
- In [29], Simsek constructed p-adic -Dedekind sums and Hardy–Berndt type sums. In the future, we will study the properties of the twisted p-adic Dedekind sums associated with our objects of study here.
Author Contributions
Conceptualization, A.B. and Y.S. Both authors have read and agreed to the published version of the manuscript.
Funding
This research received no external funding.
Acknowledgments
This paper was supported by the Scientific Research Project Administration, Akdeniz University.
Conflicts of Interest
The authors declare no conflict of interest.
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