Abstract
We study the formulas for binomial sums of harmonic numbers of higher order Recently, Mneimneh proved that . In this paper, we find several different expressions of for .
MSC:
11B65; 11A07; 05A10; 11B50; 11B73
1. Introduction
For a positive integer r, define the n-th harmonic number of order r by
When , is the original harmonic number. In this paper, we study the formula
In [1], for a positive integer n and , it is shown that . Namely,
This relation is derived by the author from an interesting probabilistic analysis. The identity (2) is a generalization of
which has been proved in [2] in the field of symbolic computation and in [3] in finite differences. The identity (2) is a special case of a general result of Boyadzhiev [4]:
In addition, Boyadzhiev’s main result (3) has been generalized in [5] to multiple harmonic-like numbers.
The main aim of this paper is to show several different expressions of as no simple form has been found.
In fact, more different generalizations of (1) or (2) can be considered. For example, recently, in [6], the so-called hyperharmonic number generalizes the harmonic number of the order r in the formula. In [7], more generalized sums and their application to multiple polylogarithms are given. In [8], some expressions of Mneimneh-type binomial sums are established, involving multiple harmonic-type sums in terms of finite sums of Stirling numbers, Bell numbers, and some related variables, and a conjecture is proposed. Then, in [9], this conjecture is resolved and generalized, and the transformation of generalized Mneimneh-like sums is presented. When we generalize too much, a lot of interesting and essential properties may be lost. Therefore, we do not consider further generalized harmonic numbers in this paper.
2. Observation
By using the harmonic numbers to express , for , we can manually obtain the following. Some initial trials for are given below.
It is interesting to observe that the number of terms of each of the right-hand sides of is equal to the number of partitions of r (), respectively. In addition, the same terms of generalized harmonic numbers appear in [10,11]
Some Initial Trials
For observation, we calculate the expressions of for small r, one by one, using the method in [12]. Here, we mention the cases for .
When , we find the following relation. Thus, by Theorem 1 in the next section, we can obtain .
Lemma 1.
When , we find the following relation. Here, () is the falling factorial with , and denotes the (unsigned) Stirling number of the first kind, arising from the relation .
Lemma 2.
Note that
Hence, we have the following formula.
Corollary 1.
Proof of Lemma 1.
Put
Since
we have
Hence, we obtain
□
Proof of Lemma 2.
When , we have the following.
Lemma 3.
Therefore, we have the following formula.
Corollary 2.
3. Expressions (Main Results)
Let be positive integers.
Theorem 1.
Theorem 2.
For ,
() can be expressed in terms of the determinant [13] ([Ch. I S2]). See also [14,15].
Theorem 3.
Remark 1.
By using the inversion formula (see, e.g., ([Lemma 1] [16]), ([13] (p. 28)) regarding (12) below, we also have
() can be expressed by a combinatorial sum ([Proposition 1 (17)] [11]):
Theorem 4.
Remember that the (complete exponential) Bell polynomial is defined by
(see, e.g., ([Ch.3.3] [17])). That is,
with . Here, the second sum satisfies the following conditions:
Theorem 5.
For , we have
4. Proof
Proof of Theorem 1.
Proof of Theorem 2.
By Theorem 1,
Hence, by , we have
□
In order to prove Theorem 4 and Theorem 3, we need the following relations.
Lemma 4.
For the sequences and , we have
Proof.
The last identity is a simple modification of Trudi’s formula (([18] (Volume 3, p. 214)), [19]):
Notice that the expansion of the second determinant is equivalent to the following relation:
Byapplying the inversion formula (see, e.g., ([Lemma 1] [16])), we can obtain the first identity. □
Proof of Theorem 3.
Proof of Theorem 4.
The result follows from the second part of Lemma 4 by setting and , satisfying (12). □
Proof of Theorem 5.
Since Bell polynomials satisfy the following recurrence relation:
(see, e.g., [17]), by setting , we have
Since
for , we can write the form in Theorem 5. □
Author Contributions
Writing—original draft preparation, T.K. and B.S.; writing—review and editing, T.K. and B.S. All authors have read and agreed to the published version of the manuscript.
Funding
This research received no external funding.
Data Availability Statement
The data are contained within the article.
Acknowledgments
The authors thank the referees for carefully reading the manuscript and providing some important related papers. This work was partly completed during the first author’s visit to the Indian Statistical Institute Bangalore, India, in July–August 2023. He is grateful for the second author’s hospitality.
Conflicts of Interest
The authors declare no conflicts of interest.
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