Next Article in Journal
Performance Optimization with LPV Synthesis for Disturbance Attenuation in Planar Motors
Next Article in Special Issue
On Symmetrical Sonin Kernels in Terms of Hypergeometric-Type Functions
Previous Article in Journal
Dynamic Programming-Based Approach to Model Antigen-Driven Immune Repertoire Synthesis
Previous Article in Special Issue
On the Containment of the Unit Disc Image by Analytical Functions in the Lemniscate and Nephroid Domains
 
 
Font Type:
Arial Georgia Verdana
Font Size:
Aa Aa Aa
Line Spacing:
Column Width:
Background:
Article

Some Symmetry and Duality Theorems on Multiple Zeta(-Star) Values

1
Department of Mathematics, University of Taipei, Taipei 100234, Taiwan
2
Department of Mathematics, National Chung Cheng University, Chia-Yi 62145, Taiwan
3
Executive Master of Business Administration, Chang Jung Christian University, Tainan City 71101, Taiwan
*
Author to whom correspondence should be addressed.
Mathematics 2024, 12(20), 3292; https://doi.org/10.3390/math12203292
Submission received: 27 September 2024 / Revised: 14 October 2024 / Accepted: 18 October 2024 / Published: 20 October 2024
(This article belongs to the Special Issue Polynomials: Theory and Applications, 2nd Edition)

Abstract

:
In this paper, we provide a symmetric formula and a duality formula relating multiple zeta values and zeta-star values. We find that the summation a + b = r 1 ( 1 ) a ζ ( a + 2 , { 2 } p 1 ) ζ ( { 1 } b + 1 , { 2 } q ) equals ζ ( { 2 } p , { 1 } r , { 2 } q ) + ( 1 ) r + 1 ζ ( { 2 } q , r + 2 , { 2 } p 1 ) . With the help of this equation and Zagier’s ζ ( { 2 } p , 3 , { 2 } q ) formula, we can easily determine ζ ( { 2 } p , 1 , { 2 } q ) and several interesting expressions.

1. Introduction

For an r-tuple α = ( α 1 , α 2 , , α r ) of positive integers with α r 2 , a multiple zeta value ζ ( α ) and a multiple zeta-star value ζ ( α ) are defined to be [1,2,3]
ζ ( α ) = 1 k 1 < k 2 < < k r k 1 α 1 k 2 α 2 k r α r , a n d ζ ( α ) = 1 k 1 k 2 k r k 1 α 1 k 2 α 2 k r α r .
We denote the parameters w ( α ) = | α | = α 1 + α 2 + + α r , d ( α ) = r , and h ( α ) = # { i α i > 1 , 1 i r } , called, respectively, the weight, the depth, and the height of α (or of ζ ( α ) , or of ζ ( α ) ). We let { a } k be k repetitions of a such that ζ ( 2 , { 3 } 3 ) = ζ ( 2 , 3 , 3 , 3 ) .
In this paper, we investigate the functions Z U (Schur multiple zeta values of anti-hook type), Z L (Schur multiple zeta values of hook type), and Z B [4,5,6]:
Z U α β : = 1 k 1 < k 2 < < k r k 1 α 1 k 2 α 2 k r α r 1 1 2 m k r 1 β 1 2 β 2 m β m , Z L α β : = 1 k 1 < k 2 < < k r k 1 α 1 k 2 α 2 k r α r k 1 1 2 m 1 β 1 2 β 2 m β m , Z B α β : = 1 k 1 < k 2 < < k r k 1 α 1 k 2 α 2 k r α r k 1 1 2 m k r 1 β 1 2 β 2 m β m .
For the sake of convergence, the functions Z U and Z B are restricted by α r 2 , and the function Z L is restricted by α r 2 , β m 2 .
Yamamoto [7] introduced a combinatorial generalization of the iterated integral, the integral associated with a 2-poset. Kaneko and Yamamoto [8] conjectured that the following integral-series identity is sufficient to describe all the linear relations of multiple zeta values over Q .
Mathematics 12 03292 i001
where the left-hand side of the above identity is an integral associated with a 2-posets introduced by Yamamoto [7] (we will introduce the associated notations in Section 2).
The use of Yamamoto’s integral is prevalent among researchers studying multiple zeta values and multiple zeta-star values [8,9,10].
Many scholars have conducted research on the function Z U appearing on the right-hand side of the above identity [4,5,8,11,12].
We simplify our notations with
α i , j = ( α i + 1 , α i + 2 , , α j ) , α i , j = ( α j , α j 1 , , α i + 1 ) ,
for i < j . Note that if i j , we set α i , j = α i , j = . For brevity, we use the lowercase English letters and lowercase Greek letters, with or without subscripts, in summations to represent non-negative and positive integers, unless otherwise specified. To make the symbols more compact, we adopt the fact ζ ( ) = ζ ( ) = 1 .
We use Yamamoto’s integral to obtain the following symmetric form between multiple zeta(-star) values in Section 3.
Theorem 1.
Let r , m , θ be nonnegative integers with θ 2 , and the vectors α = ( α 1 , α 2 , , α r ) , β = ( β 1 , β 2 , , β m ) with α i 2 , β m 2 , for 1 i r . Then
a + b = r c + d = m ( 1 ) a + c ζ ( α 0 , b ) ζ ( β 0 , c , θ , α b , r ) ζ ( β c , m ) = ζ ( α , θ , β ) ,
a + b = r c + d = m ( 1 ) a + c ζ ( α 0 , b ) ζ ( β 0 , c , θ , α b , r ) ζ ( β c , m ) = ζ ( α , θ , β ) .
The following symmetric formula that we have is truly exquisite.
Corollary 1.
For any nonnegative integers p , q , s , t , α with s 2 , t 2 , θ 2 , we have
a + b = q c + d = p ( 1 ) a + c ζ ( { s } b ) ζ ( { s } a , θ , { t } c ) ζ ( { t } d ) = ζ ( { t } p , θ , { s } q ) , a + b = q c + d = p ( 1 ) a + c ζ ( { s } b ) ζ ( { s } a , θ , { t } c ) ζ ( { t } d ) = ζ ( { t } p , θ , { s } q ) .
We note that a version of finite sums of the above two identities can be found in [13,14].
Let ( a 1 , b 1 ) , ( a 2 , b 2 ) , , ( a n , b n ) be n pairs of nonnegative integers. If we write
( α 1 , α 2 , , α r ) = ( { 1 } a 1 , b 1 + 2 , { 1 } a 2 , b 2 + 2 , , { 1 } a n , b n + 2 )
and set
( { 1 } b n , a n + 2 , { 1 } b n 1 , a n 1 + 2 , , { 1 } b 1 , a 1 + 2 ) = ( β 1 , β 2 , , β m ) ,
then the duality theorem of multiple zeta values [15] is stated as
ζ ( α 1 , α 2 , , α r ) = ζ ( β 1 , β 2 , , β m ) .
We say that ζ ( β 1 , , β m ) is the dual of ζ ( α 1 , , α r ) , and we denote it as ζ ( α 1 , , α r ) = ζ ( β 1 , , β m ) .
In 2015, the first author [4] gave a formula related to Z U :
Z U β 1 , β 2 , , β m { 1 } q = | d | = q ζ ( α 1 + d 1 , , α r + d r ) j = 1 r α j + d j 1 d j ,
if ζ ( β 1 , , β m ) is the dual of ζ ( α 1 , , α r ) .
In Section 4, we present three different methods to prove the following duality theorem between these Z B , Z U , and Z L functions.
Theorem 2.
If ζ ( β 1 , β 2 , , β m ) is the dual of ζ ( α 1 , α 2 , , α r ) . Given any nonnegative integer n, we have
Z U α 1 , α 2 , , α r { 2 } n = Z L β 1 , β 2 , , β m { 2 } n , a n d Z B α 1 , α 2 , , α r { 2 } n = Z B β 1 , β 2 , , β m { 2 } n .
Chen and Eie [5] use these three functions to give three new sum formulas for multiple zeta(-star) values with height 2 and the evaluation of ζ ( { 1 } m , { 2 } n + 1 ) . For example, the authors use Z B to obtain (Theorem 1.1, [5])
α 1 + α 2 = n α 1 , α 2 1 ζ ( α 1 , { 1 } m , α 2 + 1 ) = ( m + n ) ζ ( m + n + 1 ) .
We use the duality theorem on the functions Z U and Z L to obtain the following formula.
Theorem 3.
For any nonnegative integers p, q, and r with p > 0 , q > 0 , we have
ζ ( { 2 } p , { 1 } r , { 2 } q ) + ( 1 ) r + 1 ζ ( { 2 } q , r + 2 , { 2 } p 1 ) = a + b = r 1 ( 1 ) a ζ ( a + 2 , { 2 } p 1 ) ζ ( { 1 } b + 1 , { 2 } q ) .
Substituting r = 1 into the above equation yields Equation (2) in [13]. By employing this in conjunction with Zagier’s formula (ref. [16]) for computing ζ ( { 2 } p , 3 , { 2 } q ) , we can determine the values of ζ ( { 2 } p , 1 , { 2 } q ) :
ζ ( { 2 } p , 1 , { 2 } q ) = 2 k = 1 p + q 2 k 2 q 1 1 2 2 k 2 k 2 p 1 ζ ( { 2 } p + q k ) ζ ( 2 k + 1 ) ,
for any positive integers p and q and this result coincides with Theorem 1.6 in [13]. We will discuss Theorem 3 and its relevant applications in the final section, providing some intriguing formulas.

2. Some Preliminaries and Auxiliary Tools

In this section, we review the definitions and basic properties of 2-labeled posets (in this paper, we call them 2-posets for short) and the associated integrals first introduced by Yamamoto [7].
Definition 1
(Definition 3.1, [8]). A 2-poset is a pair ( X , δ X ) , where X = ( X , ) is a finite partially ordered set (poset for short) and δ X is a map from X to { 0 , 1 } . We often omit δ X and simply say “a 2-poset X.” The δ X is called the label map of X.
A 2-poset ( X , δ X ) is called admissible if δ X ( x ) = 0 for all maximal elements x X and δ X ( x ) = 1 for all minimal elements x X .
A 2-poset is depicted as a Hasse diagram in which an element x with δ ( x ) = 0 (resp. δ ( x ) = 1 ) is represented by ∘ (resp. •). For example, the diagram
Mathematics 12 03292 i002
represents the 2-poset X = { x 1 , x 2 , x 3 , x 4 , x 5 } with order x 1 < x 2 < x 3 > x 4 < x 5 and label ( δ X ( x 1 ) , , δ X ( x 5 ) ) = ( 1 , 0 , 0 , 1 , 0 ) .
Definition 2
(Definition 3.2, [8]). For an admissible 2-poset X, we define the associated integral
I ( X ) = Δ X x X ω δ X ( x ) ( t x ) ,
where
Δ X = ( t x ) x [ 0 , 1 ] X | t x < t y if x < y a n d ω 0 ( t ) = d t t , ω 1 ( t ) = d t 1 t .
Note that the admissibility of a 2-poset corresponds to the convergence of the associated integral.
Example 1.
When an admissible 2-poset is totally ordered, the corresponding integral is exactly the iterated integral expression for a multiple zeta value. To be precise, for an index α = ( α 1 , , α r ) (admissible or not), we write the ‘totally ordered’ diagram:
Mathematics 12 03292 i003
In [7], an integral expression for multiple zeta-star values is described in terms of a 2-poset. For an index β = ( β 1 , β 2 , , β m ) , we write the following diagram:
Mathematics 12 03292 i004
Then, if α and β are admissible, we have [10] Proposition 2.4, 2.7
Mathematics 12 03292 i005
For example,
Mathematics 12 03292 i006
We also recall an algebraic setup for 2-posets (cf. Remark at the end of §2 of [7]). Let P be the Q -algebra generated by the isomorphism classes of 2-posets, whose multiplication is given by the disjoint union of 2-posets. Then, the integral (4) defines a Q -algebra homomorphism I : P 0 R from the subalgebra P 0 of P generated by the classes of admissible 2-posets.
Following these notations, we have
Mathematics 12 03292 i007
In fact, the upper left equation is the same as (Theorem 4.1, [8]). Kaneko and Yamamoto conjecture that any linear dependency of MZVs over Q is deduced from this equation.
We evaluate Z L 1 , 2 1 , 2 as an example: Let D = { ( t 1 , t 2 , t 3 , t 4 , t 5 , t 6 ) [ 0 , 1 ] 6 t 1 < t 2 > t 3 > t 4 < t 5 < t 6 } , we calculate
Mathematics 12 03292 i008
We need some properties of these three functions Z U , Z L and Z B , please see [5] for details:
ζ ( α ) ζ ( β ) = Z L α 1 , α 2 , , α r β 1 , β 2 , , β m + Z L β 1 , α 1 , , α r β 2 , β 3 , , β m ,
ζ ( α ) ζ ( β ) = Z U α 1 , α 2 , , α r β 1 , β 2 , , β m + Z U α 1 , , α r , β m β 1 , , β m 1 .
Proposition 1
(Proposition 4.1, [5]). For an r-tuple α = ( α 1 , α 2 , , α r ) of positive integers with α 1 2 , α r 2 , we have
k = 0 r ( 1 ) k ζ ( α k , α k 1 , , α 1 ) ζ ( α k + 1 , α k + 2 , , α r ) = 1 , i f r = 0 , 0 , o t h e r w i s e .
Let α = ( s , , s ) = ( { s } r ) in Equation (9). We obtain the classical known result (Equation (5.8), [5])
a + b = r ( 1 ) a ζ ( { s } a ) ζ ( { s } b ) = 1 , i f   r = 0 , 0 , o t h e r w i s e .
We derive an evaluation of Z L using Equation (7).
Z L α 1 , , α r β 1 , , β m = ζ ( α 1 , , α r ) ζ ( β 1 , , β m ) Z L β 1 , α 1 , , α r β 2 , , β m = ζ ( α 1 , , α r ) ζ ( β 1 , , β m ) ζ ( β 1 , α 1 , , α r ) ζ ( β 2 , , β m ) + ( 1 ) 2 Z L β 2 , β 1 , α 1 , , α r β 3 , , β m .
We use Equation (7) repeatedly until the vector in the second row is the empty set. Since
Z L β m , β m 1 , , β 1 , α 1 , , α r = ζ ( β m , β m 1 , , β 1 , α 1 , , α r ) ,
we arrive a formula for the function Z L :
Z L α β = a + b = m ( 1 ) a ζ ( β a , , β 1 , α 1 , , α r ) ζ ( β a + 1 , , β m ) .
If we use Equation (7) in a different direction
Z L α 1 , , α r β 1 , , β m = ζ ( α 2 , , α r ) ζ ( α 1 , β 1 , , β m ) Z L α 2 , , α r α 1 , β 1 , β 2 , , β m ,
then we obtain the following formula for Z L .
Z L α 1 , , α r β 1 , , β m = a + b = r 1 ( 1 ) a ζ ( α a + 2 , , α r ) ζ ( α a + 1 , , α 1 , β 1 , , β m ) .
Similarly, we also use Equation (8) to obtain two formulas of the function Z U . We conclude these four formulas in the following propositions.
Proposition 2.
For any nonnegative integers m , r , an r-tuple α = ( α 1 , α 2 , , α r ) of positive integers, and an m-tupe β = ( β 1 , β 2 , , β m ) of positive integers, with α r 2 , β m 2 , we have
Z L α β = a + b = m ( 1 ) a ζ ( β a , , β 1 , α 1 , , α r ) ζ ( β a + 1 , , β m )                  
= a + b = r 1 ( 1 ) a ζ ( α a + 2 , , α r ) ζ ( α a + 1 , , α 1 , β 1 , , β m ) .
And
Z U α β = a + b = m ( 1 ) a ζ ( α 1 , , α r , β m , , β b + 1 ) ζ ( β 1 , , β b )                  
= a + b = r 1 ( 1 ) a ζ ( α 1 , , α b ) ζ ( β 1 , , β m , α r , , α b + 1 ) ,
where β i 2 ( 1 i m ) for Equation (13) and α j 2 ( 1 j r ) for Equation (14).
We use a formula among the function Z B and Z U (Proposition 7.1, [5])
( 1 ) m Z B α m + 1 , , α r α m , , α 1 = ζ ( α ) + k = 1 m ( 1 ) k Z U α k + 1 , , α r α k , , α 1 ,
where α r 2 and 1 m r , and Equation (13) to obtain an explicit formula for the function Z B :
Z B α m + 1 , , α r α m , , α 1 = 0 j d m ( 1 ) m + j d ζ ( α d + 1 , , α r , α 1 , , α j ) ζ ( α d , , α j + 1 ) .

3. Symmetric Formulas and Theorem 1

In order to prove Theorem 1, we apply Yamamoto’s integrals to show four equalities that involve the Z U and Z L functions.
Proposition 3
(ref. [8]). For any nonnegative integers m , r , θ with θ 2 , an r-tuple α = ( α 1 , α 2 , , α r ) of positive integers, and an m-tupe β = ( β 1 , β 2 , , β m ) of positive integers with β m 2 , we have
k = 0 m ( 1 ) k ζ ( β k , m ) Z U α β 0 , k = ζ ( α , β ) , f o r   α r 2 ,             
k = 0 r ( 1 ) r k ζ ( α 0 , k ) Z L β α k , r = ζ ( α , β ) , f o r   α i 2 , 1 i r ,
k = 0 m ( 1 ) k ζ ( β k , m ) Z U β 0 , k , θ α = ζ ( α , θ , β ) ,                                    
k = 0 r ( 1 ) r k ζ ( α 0 , k ) Z L θ , α k , r β = ζ ( α , θ , β ) , f o r   α i 2 , 1 i r .
Proof. 
We present the process to get obtain the equation, the other equations are obtained similarly. Since ζ ( α , β ) can be represented as
Mathematics 12 03292 i009
Since for an integer i with 1 i m , we have
Mathematics 12 03292 i010
Continue this process we have
Mathematics 12 03292 i011
Substituing into the original equation, we get the conclusion. □
We can easily derive the identities in Theorem 1 using the equations from Proposition 3. First we substitute the representation Equation (13) of Z U :
Z U β 0 , k , θ α = a + b = r ( 1 ) a ζ ( β 0 , k , θ , α b , r ) ζ ( α 0 , b )
into Equation (19), we have Equation (1). The other formula Equation (2) is obtained from Equation (17):
c + d = m ( 1 ) c ζ ( β c , m ) Z U α , θ β 0 , c = ζ ( α , θ , β ) ,
using the representation Equation (14) of Z U :
a + b = r ( 1 ) a ζ ( α 0 , b ) ζ ( β 0 , c , θ , α b , r ) .
Therefore, we complete the proof of Theorem 1.
Furthermore, the beautiful equations in Corollary 1 are derived by substituting α = { t } p and β = { s } q into Theorem 1.

4. Duality Theorems and Theorem 2

We will begin by proving the first equation in Theorem 2.
Theorem 4.
Let ζ ( β ) be the dual of ζ ( α ) and n be a nonnegative integer. Then
Z U α { 2 } n = Z L β { 2 } n .
For this theorem, we provide three different methods of proof.
Method 
1—The generating functions. We let G α ( x ) , g α ( x ) be the generating function of Z U α { 2 } n , Z L α { 2 } n , respectively, that is,
G α ( x ) = n = 0 Z U α { 2 } n x 2 n , a n d g α ( x ) = n = 0 Z L α { 2 } n x 2 n .
We begin from the generating function G α ( x ) .
G α ( x ) = 1 k 1 < k 2 < < k r 1 j k r 1 x 2 j 2 1 k 1 α 1 k 2 α 2 k r α r = π x sin ( π x ) 1 k 1 < k 2 < < k r j > k r 1 x 2 j 2 k 1 α 1 k 2 α 2 k r α r = π x sin ( π x ) n = 0 ( 1 ) n ζ ( α 1 , α 2 , , α r , { 2 } n ) x 2 n .
Since the dual of ζ ( α ) is ζ ( β ) , we have
ζ ( α , { 2 } n ) = ζ ( { 2 } n , β ) .
Therefore, the generating function G α ( x ) can be rewritten as
π x sin ( π x ) 1 1 < 2 < < m 1 j < 1 1 x 2 j 2 1 β 1 2 β 2 m β m = 1 1 < 2 < < m 1 j 1 x 2 j 2 1 1 β 1 2 β 2 m β m = g β ( x ) .
The coefficients of x 2 n of both generating functions give our identity.
Method 
2—Yamamoto’s integral. Since the duality of the Euler sums is represented by u i = 1 t i in its Drinfel’d iterated integral, the corresponding 2-poset Hasse diagram appears as a vertical reflection, with ∘ and • interchanged.
Mathematics 12 03292 i012
We explain it by an example with Z U 3 , 3 2 , 2 # = Z L 1 , 2 , 1 , 2 2 , 2 .
Mathematics 12 03292 i013
Method 
3—Expressions by MZVs and MZSVs. We use Equations (13) and (11), we know that
Z U α { 2 } n = a + b = n ( 1 ) a ζ ( α , { 2 } a ) ζ ( { 2 } b ) , Z L β { 2 } n = a + b = n ( 1 ) a ζ ( { 2 } a , β ) ζ ( { 2 } b ) .
Since ζ ( α ) = ζ ( β ) , this implies that ζ ( α , { 2 } a ) = ζ ( { 2 } a , β ) . Thus, we have
Z U α { 2 } n = a + b ζ ( α , { 2 } a ) ζ ( { 2 } b ) = a + b ζ ( { 2 } a , β ) ζ ( { 2 } b ) = Z L β { 2 } n .
Next, we proceed to prove the second equation of Theorem 2.
Using Equation (16), we know that
Z B α { 2 } m = a + b + c = m ( 1 ) a + b ζ ( { 2 } a , α , { 2 } b ) ζ ( { 2 } c ) .
It is easy to see that ζ ( { 2 } a , α , { 2 } b ) = ζ ( { 2 } b , β , { 2 } a ) , we have
Z B α { 2 } n = a + b + c = n ( 1 ) a + b ζ ( { 2 } a , α , { 2 } b ) ζ ( { 2 } c ) = a + b + c = n ( 1 ) a + b ζ ( { 2 } b , β , { 2 } a ) ζ ( { 2 } c ) = Z B β { 2 } n .
Therefore, the function Z B satisfies second equation. We complete the proof.
Nakasuji, Ohno (Theorem 4.4, [17]) use Schur multiple zeta functions to give a more general duality theorem. However, our particular duality forms are founded by the classical generating functions, or the new Yamamoto’s integral.
Since ζ ( k ) = ζ ( { 1 } k 2 , 2 ) , for k 2 . Then, for any nonnegative integer n, we have
ζ ( 2 n + k ) = Z B k { 2 } n = Z B { 1 } k 2 , 2 { 2 } n = a + b + c = n ( 1 ) a + b ζ ( { 2 } a , { 1 } k 2 , { 2 } b + 1 ) ζ ( { 2 } c ) .
Let k = 2 , we have the following weighted sum formula:
ζ ( 2 n + 2 ) = a + b = n ( 1 ) b ( b + 1 ) ζ ( { 2 } b + 1 ) ζ ( { 2 } a ) .

5. Theorem 3 and Some More Formulas

In this last section, we will start by providing the proof of Theorem 3, and then we will discuss some applications.
Proof of Theorem 3.
Let
G ( x ) = p = 0 ζ ( { 2 } p , { 1 } r , { 2 } q ) x 2 p
be the generating function of ζ ( { 2 } p , { 1 } r , { 2 } q ) x 2 p . Thus,
G ( x ) = 1 k 1 k 2 k q + r 1 j k 1 1 x 2 j 2 1 k 1 k 2 k r k r + 1 2 k r + 2 2 k q + r 2 = π x sin ( π x ) 1 k 1 k 2 k q + r j > k 1 1 x 2 j 2 k 1 k 2 k r k r + 1 2 k r + 2 2 k q + r 2 .
We represent the above summation as
ζ ( { 1 } r , { 2 } q ) + n = 1 ( 1 ) n Z L 1 , { 2 } n { 1 } r 1 , { 2 } q x 2 n .
By convolution, we have
G ( x ) = n = 0 ζ ( { 2 } n ) ζ ( { 1 } r , { 2 } q ) x 2 n + p = 1 m + n = p m 1 ( 1 ) m ζ ( { 2 } n ) Z L 1 , { 2 } m { 1 } r 1 , { 2 } q x 2 p .
Comparing the coefficient of x 2 p , for p 1 , we have
ζ ( { 2 } p , { 1 } r , { 2 } q ) = ζ ( { 2 } p ) ζ ( { 1 } r , { 2 } q ) + m + n = p 1 ( 1 ) m + 1 ζ ( { 2 } n ) Z L 1 , { 2 } m + 1 { 1 } r 1 , { 2 } q .
We use Equation (7) to the function Z L , this gives
Z L 1 , { 2 } m + 1 { 1 } r 1 , { 2 } q = ( 1 ) r 1 Z L { 1 } r , { 2 } m + 1 { 2 } q + a + b = r 2 ( 1 ) a ζ ( { 1 } a + 1 , { 2 } m + 1 ) ζ ( { 1 } b + 1 , { 2 } q ) .
It is clear that ζ ( { 1 } a + 1 , { 2 } m + 1 ) = ζ ( { 2 } m , a + 3 ) , and we apply the dual theorem to transform
Z L { 1 } r , { 2 } m + 1 { 2 } q = Z U { 2 } m , r + 2 { 2 } q
then we obtain
Z L 1 , { 2 } m + 1 { 1 } r 1 , { 2 } q = ( 1 ) r 1 Z U { 2 } m , r + 2 { 2 } q + a + b = r 2 ( 1 ) a ζ ( { 2 } m , a + 3 ) ζ ( { 1 } b + 1 , { 2 } q ) .
The summation in Equation (23) becomes
m + n = p 1 ( 1 ) m + r ζ ( { 2 } n ) Z U { 2 } m , r + 2 { 2 } q + m + n = p 1 a + b = r 2 ( 1 ) m + a + 1 ζ ( { 2 } n ) ζ ( { 2 } m , a + 3 ) ζ ( { 1 } b + 1 , { 2 } q ) .
The second summation of the above formula can be simplified by using Equation (9)
m + n = p 1 ( 1 ) m ζ ( { 2 } n ) ζ ( { 2 } m , a + 3 ) = ζ ( a + 3 , { 2 } p 1 ) .
We will obtain
a + b = r 2 ( 1 ) a + 1 ζ ( a + 3 , { 2 } p 1 ) ζ ( { 1 } b + 1 , { 2 } q ) .
It remains to treat the summation
m + n = p 1 ( 1 ) m + r ζ ( { 2 } n ) Z U { 2 } m , r + 2 { 2 } q .
We apply Equation (19) with α = ( { 2 } q ) , θ = r + 2 , and β = ( { 2 } p 1 ) , then the above summation is equal to
( 1 ) r ζ ( { 2 } q , r + 2 , { 2 } p 1 ) .
Therefore, Equation (23) becomes
ζ ( { 2 } p , { 1 } r , { 2 } q ) = ζ ( { 2 } p ) ζ ( { 1 } r , { 2 } q ) + ( 1 ) r ζ ( { 2 } q , r + 2 , { 2 } p 1 ) + a + b = r 2 ( 1 ) a + 1 ζ ( a + 3 , { 2 } p 1 ) ζ ( { 1 } b + 1 , { 2 } q ) = ( 1 ) r ζ ( { 2 } q , r + 2 , { 2 } p 1 ) + a + b = r 1 ( 1 ) a ζ ( a + 2 , { 2 } p 1 ) ζ ( { 1 } b + 1 , { 2 } q ) .
This finishes our work. □
It is well-known that (ref. [18]) ζ ( 1 , { 2 } q ) = 2 ζ ( 2 q + 1 ) , and we leverage Zagier’s formula (ref. [16]) to compute ζ ( { 2 } q , 3 , { 2 } p 1 ) :
ζ ( { 2 } q , 3 , { 2 } p 1 ) = 2 k = 1 p + q 2 k 2 q δ k , q 1 1 2 2 k 2 k 2 p 1 ζ ( { 2 } p + q k ) ζ ( 2 k + 1 ) .
By substituting r = 1 in Equation (3), we obtain an evaluation of ζ ( { 2 } p , 1 , { 2 } q ) , for any positive integers p and q (Theorem 1.6, [13]):
ζ ( { 2 } p , 1 , { 2 } q ) = 2 k = 1 p + q 2 k 2 q 1 1 2 2 k 2 k 2 p 1 ζ ( { 2 } p + q k ) ζ ( 2 k + 1 ) .
On the other hand, if we apply p = q = 1 in Equation (3), then
a + b = r ( 1 ) a ( b + 1 ) ζ ( a + 2 ) ζ ( b + 2 ) = ζ ( 2 , { 1 } r , 2 ) + ( 1 ) r ζ ( r + 2 , 2 ) ,
for any nonnegative integer r, by using the fact (ref. [5]) ζ ( { 1 } b + 1 , 2 ) = ( b + 2 ) ζ ( b + 3 ) .

Author Contributions

Conceptualization, K.-W.C. and M.E.; methodology, K.-W.C. and M.E.; validation, K.-W.C.; data curation, Y.L.O.; writing—original draft preparation, K.-W.C. and M.E.; writing—review and editing, K.-W.C.; funding acquisition, K.-W.C. All authors have read and agreed to the published version of the manuscript.

Funding

The first author was funded by the Ministry of Science and Technology, Taiwan, R.O.C., under grant number MOST 111-2115-M-845-001, and also by the National Science and Technology Council, Taiwan, R.O.C., under grant NSTC 113-2115-M-845-001.

Data Availability Statement

Data are contained within the article.

Conflicts of Interest

The authors declare no conflicts of interest.

References

  1. Hoffman, M.E. Multiple harmonic series. Pac. J. Math. 1992, 152, 275–290. [Google Scholar] [CrossRef]
  2. Ohno, Y. Sum relations for multiple zeta values. In Zeta Functions, Topology and Quantum Physics, Developments in Mathematics; Aoki, T., Kanemitsu, S., Nakahara, M., Ohno, Y., Eds.; Springer: Boston, MA, USA, 2005; Volume 14, pp. 131–144. [Google Scholar]
  3. Zagier, D. Values of zeta functions and their applications. In First European Congress of Mathematics Paris; Birkhäuser: Baesl, Switzerland, 1994; Volume II, pp. 497–512. [Google Scholar]
  4. Chen, K.-W. Generalized harmonic numbers and Euler sums. Int. J. Number Theory 2017, 13, 513–528. [Google Scholar] [CrossRef]
  5. Chen, K.-W.; Eie, M. On three general forms of multiple zeta(-star) values. Expo. Math. 2023, 41, 299–315. [Google Scholar] [CrossRef]
  6. Chen, K.-W.; Chung, C.-L.; Eie, M. Sum formulas and duality theorems of multiple zeta values. J. Number Theory 2016, 158, 33–53. [Google Scholar] [CrossRef]
  7. Yamamoto, S. Multiple zeta-star values and multiple integrals. RIMS Kôky r ̂ oku Bessatsu 2017, B68, 3–14. [Google Scholar]
  8. Kaneko, M.; Yamamoto, S. A new integral-series identity of multiple zeta values and regularizations. Sel. Math. New Ser. 2018, 24, 2499–2521. [Google Scholar] [CrossRef]
  9. Hirose, M.; Murahara, H.; Ono, M. On variants of symmetric multiple zeta-star values and the cyclic sum formula. Ramanujan J. 2021, 56, 467–489. [Google Scholar] [CrossRef]
  10. Yamamoto, S. Integrals associated with 2-posets and applications to multiple zeta values. RIMS Kôky r ̂ oku Bessatsu 2020, B83, 27–46. [Google Scholar]
  11. Nakasuji, M.; Phuksuwan, O.; Yamasaki, Y. On Schur multiple zeta functions: A combinatoric generalization of multiple zeta functions. Adv. Math. 2018, 333, 570–619. [Google Scholar] [CrossRef]
  12. Nakasuji, M.; Takeda, W. Shuffle product formula of the Schur multiple zeta values of hook type. arXiv 2022, arXiv:2202.01402v2. [Google Scholar]
  13. Tasaka, K.; Yamamoto, S. On some multiple zeta-star values of one-two-three indices. Inter. J. Number Theory 2013, 9, 1171–1184. [Google Scholar] [CrossRef]
  14. Xu, C. Evaluations of nonlinear Euler sums of weight ten. Appl. Math. Comput. 2019, 346, 594–611. [Google Scholar] [CrossRef]
  15. Ohno, Y. A generalization of the duality and sum formulas on the multiple zeta values. J. Number Theory 1999, 74, 39–43. [Google Scholar] [CrossRef]
  16. Zagier, D. Evaluation of the multiple zeta value ζ(2,,2,3,2,,2). Ann. Math. 2012, 175, 977–1000. [Google Scholar] [CrossRef]
  17. Nakasuji, M.; Ohno, Y. Duality formula and its generalization for Schur multiple zeta functions. arXiv 2019, arXiv:2109.14362v1. [Google Scholar]
  18. Zlobin, S.A. Generating functions for the values of a multiple zeta function. Vestnik Moskov. Univ. Ser. 1 Mat. Mekh. 2005, 2, 55–59. [Google Scholar]
Disclaimer/Publisher’s Note: The statements, opinions and data contained in all publications are solely those of the individual author(s) and contributor(s) and not of MDPI and/or the editor(s). MDPI and/or the editor(s) disclaim responsibility for any injury to people or property resulting from any ideas, methods, instructions or products referred to in the content.

Share and Cite

MDPI and ACS Style

Chen, K.-W.; Eie, M.; Ong, Y.L. Some Symmetry and Duality Theorems on Multiple Zeta(-Star) Values. Mathematics 2024, 12, 3292. https://doi.org/10.3390/math12203292

AMA Style

Chen K-W, Eie M, Ong YL. Some Symmetry and Duality Theorems on Multiple Zeta(-Star) Values. Mathematics. 2024; 12(20):3292. https://doi.org/10.3390/math12203292

Chicago/Turabian Style

Chen, Kwang-Wu, Minking Eie, and Yao Lin Ong. 2024. "Some Symmetry and Duality Theorems on Multiple Zeta(-Star) Values" Mathematics 12, no. 20: 3292. https://doi.org/10.3390/math12203292

APA Style

Chen, K.-W., Eie, M., & Ong, Y. L. (2024). Some Symmetry and Duality Theorems on Multiple Zeta(-Star) Values. Mathematics, 12(20), 3292. https://doi.org/10.3390/math12203292

Note that from the first issue of 2016, this journal uses article numbers instead of page numbers. See further details here.

Article Metrics

Back to TopTop