Hyperharmonic number

In mathematics, the n-th hyperharmonic number of order r, denoted by ${\displaystyle H_{n}^{(r)}}$, is recursively defined by the relations:

${\displaystyle H_{n}^{(0)}={\frac {1}{n}},}$

and

${\displaystyle H_{n}^{(r)}=\sum _{k=1}^{n}H_{k}^{(r-1)}\quad (r>0).}$^{[citation needed]}

In particular, ${\displaystyle H_{n}=H_{n}^{(1)}}$ is the n-th harmonic number.

The hyperharmonic numbers were discussed by J. H. Conway and R. K. Guy in their 1995 book The Book of Numbers.^[1]: 258

Identities involving hyperharmonic numbers

By definition, the hyperharmonic numbers satisfy the recurrence relation

${\displaystyle H_{n}^{(r)}=H_{n-1}^{(r)}+H_{n}^{(r-1)}.}$

In place of the recurrences, there is a more effective formula to calculate these numbers:

${\displaystyle H_{n}^{(r)}={\binom {n+r-1}{r-1}}(H_{n+r-1}-H_{r-1}).}$

The hyperharmonic numbers have a strong relation to combinatorics of permutations. The generalization of the identity

${\displaystyle H_{n}={\frac {1}{n!}}\left[{n+1 \atop 2}\right].}$

reads as

${\displaystyle H_{n}^{(r)}={\frac {1}{n!}}\left[{n+r \atop r+1}\right]_{r},}$

where ${\displaystyle \left[{n \atop r}\right]_{r}}$ is an r-Stirling number of the first kind.^[2]

Asymptotics

The above expression with binomial coefficients easily gives that for all fixed order r>=2 we have.^[3]

${\displaystyle H_{n}^{(r)}\sim {\frac {1}{(r-1)!}}\left(n^{r-1}\ln(n)\right),}$

that is, the quotient of the left and right hand side tends to 1 as n tends to infinity.

An immediate consequence is that

${\displaystyle \sum _{n=1}^{\infty }{\frac {H_{n}^{(r)}}{n^{m}}}<+\infty }$

when m>r.

Generating function and infinite series

The generating function of the hyperharmonic numbers is

${\displaystyle \sum _{n=0}^{\infty }H_{n}^{(r)}z^{n}=-{\frac {\ln(1-z)}{(1-z)^{r}}}.}$

The exponential generating function is much more harder to deduce. One has that for all r=1,2,...

${\displaystyle \sum _{n=0}^{\infty }H_{n}^{(r)}{\frac {t^{n}}{n!}}=e^{t}\left(\sum _{n=1}^{r-1}H_{n}^{(r-n)}{\frac {t^{n}}{n!}}+{\frac {(r-1)!}{(r!)^{2}}}t^{r}\,_{2}F_{2}\left(1,1;r+1,r+1;-t\right)\right),}$

where ₂F₂ is a hypergeometric function. The r=1 case for the harmonic numbers is a classical result, the general one was proved in 2009 by I. Mező and A. Dil.^[4]

The next relation connects the hyperharmonic numbers to the Hurwitz zeta function:^[3]

${\displaystyle \sum _{n=1}^{\infty }{\frac {H_{n}^{(r)}}{n^{m}}}=\sum _{n=1}^{\infty }H_{n}^{(r-1)}\zeta (m,n)\quad (r\geq 1,m\geq r+1).}$

Integer hyperharmonic numbers

It is known, that the harmonic numbers are never integers except the case n=1. The same question can be posed with respect to the hyperharmonic numbers: are there integer hyperharmonic numbers? István Mező proved^[5] that if r=2 or r=3, these numbers are never integers except the trivial case when n=1. He conjectured that this is always the case, namely, the hyperharmonic numbers of order r are never integers except when n=1. This conjecture was justified for a class of parameters by R. Amrane and H. Belbachir.^[6] Especially, these authors proved that ${\displaystyle H_{n}^{(4)}}$ is not integer for all r<26 and n=2,3,... Extension to high orders was made by Göral and Sertbaş.^[7] These authors have also shown that ${\displaystyle H_{n}^{(r)}}$ is never integer when n is even or a prime power, or r is odd.

Another result is the following.^[8] Let ${\displaystyle S(x)}$ be the number of non-integer hyperharmonic numbers such that ${\displaystyle (n,x)\in [0,x]\times [0,x]}$. Then, assuming the Cramér's conjecture,

${\displaystyle S(x)=x^{2}+O(x\log ^{3}x).}$

Note that the number of integer lattice points in ${\displaystyle [0,x]\times [0,x]}$ is ${\displaystyle x^{2}+O(x^{2})}$, which shows that most of the hyperharmonic numbers cannot be integer.

The problem was finally settled by D. C. Sertbaş who found that there are infinitely many hyperharmonic integers, albeit they are quite huge. The smallest hyperharmonic number which is an integer found so far is^[9]

${\displaystyle H_{33}^{(64(2^{2659}-1)+32)}.}$

External links

• Wolfram MathWorld