Abel–Dini–Pringsheim theorem

Template:Short description In calculus, the Abel–Dini–Pringsheim theorem is a convergence test which constructs from a divergent series a series that diverges more slowly, and from convergent series one that converges more slowly.Template:Rp Consequently, for every convergence test based on a particular series there is a series about which the test is inconclusive.Template:Rp For example, the Raabe test is essentially a comparison test based on the family of series whose $n$th term is $1/n^t$ (with $t\in ℝ$) and is therefore inconclusive about the series of terms $1/(n\ln n)$ which diverges more slowly than the harmonic series.

Definitions

The Abel–Dini–Pringsheim theorem can be given for divergent series or convergent series. Helpfully, these definitions are equivalent, and it suffices to prove only one case. This is because applying the Abel–Dini–Pringsheim theorem for divergent series to the series with partial sum

${S_n}^{\prime }=\frac{1}{r_n}$

yields the Abel–Dini–Pringsheim theorem for convergent series.

For divergent series

Suppose that $(a_n{)}_{n=0}^{\mathrm{\infty }}\subset (0,\mathrm{\infty })$ is a sequence of positive real numbers such that the series

$\sum _{n=0}^{\mathrm{\infty }}{a}_n=\mathrm{\infty }$

diverges to infinity. Let $S_n=a_0+a_1+\cdots +a_n$ denote the $n$th partial sum. The Abel–Dini–Pringsheim theorem for divergent series states that the following conditions hold.

1. $\sum _{n=0}^{\mathrm{\infty }}\frac{a_n}{S_n}=\mathrm{\infty }$
2. For all $ϵ>0$ we have $\sum _{n=1}^{\mathrm{\infty }}\frac{a_n}{S_n{S}_{n-1}^{ϵ}}<\mathrm{\infty }$
3. If also $\underset{n\to \mathrm{\infty }}{lim}\frac{a_n}{S_n}=0$, then $\sum _{k=0}^n\frac{a_k}{S_k}\sim \ln S_n$

Consequently, the series

$\sum _{n=0}^{\mathrm{\infty }}\frac{a_n}{S_n^t}$

converges if $t>1$ and diverges if $t\le 1$. When $t\le 1$, this series diverges less rapidly than $a_n$. Template:Math proof

For convergent series

Suppose that $(a_n{)}_{n=0}^{\mathrm{\infty }}\subset (0,\mathrm{\infty })$ is a sequence of positive real numbers such that the series

$\sum _{n=0}^{\mathrm{\infty }}{a}_n<\mathrm{\infty }$

converges to a finite number. Let $r_n=a_n+a_{n+1}+a_{n+2}+\cdots$ denote the $(n-1)$th remainder of the series. According to the Abel–Dini–Pringsheim theorem for convergent series, the following conditions hold.

• $\sum _{n=0}^{\mathrm{\infty }}\frac{a_n}{r_n}=\mathrm{\infty }$
• For all $ϵ>0$ we have $\sum _{n=0}^{\mathrm{\infty }}\frac{a_n}{r_n^{1-ϵ}}<\mathrm{\infty }$
• If also $\underset{n\to \mathrm{\infty }}{lim}\frac{a_n}{r_n}=0$ then $\underset{n\to \mathrm{\infty }}{lim}\frac{a_0/r_0+a_1/r_1+\cdots +a_n/r_n}{\ln r_n}=-1$

In particular, the series

$\sum _{n=0}^{\mathrm{\infty }}\frac{a_n}{r_n^t}$

is convergent when $t<1$, and divergent when $t\ge 1$. When $t<1$, this series converges more slowly than $a_n$.

Examples

The series

$\sum _{n=0}^{\mathrm{\infty }}1$

is divergent with the $n$th partial sum being $n$. By the Abel–Dini–Pringsheim theorem, the series

$\sum _{n=0}^{\mathrm{\infty }}\frac{1}{n^t}$

converges when $t>1$ and diverges when $t\le 1$. Since $1/n$ converges to 0, we have the asymptotic approximation

$\underset{n\to \mathrm{\infty }}{lim}\frac{1+1/2+\cdots +1/n}{\ln n}=1.$

Now, consider the divergent series

$\sum _{n=1}^{\mathrm{\infty }}\frac{1}{n}$

thus found. Apply the Abel–Dini–Pringsheim theorem but with partial sum replaced by asymptotically equivalent sequence $\ln n$. (It is not hard to verify that this can always be done.) Then we may conclude that the series

$\sum _{n=1}^{\mathrm{\infty }}\frac{1}{n{\ln }^{t}n}$

converges when $t>1$ and diverges when $t\le 1$. Since $1/(n\ln n)$ converges to 0, we have

$\underset{n\to \mathrm{\infty }}{lim}\frac{1+1/(2\ln 2)+\cdots +1/(n\ln n)}{\ln \ln n}=1.$

Historical notes

The theorem was proved in three parts. Niels Henrik Abel proved a weak form of the first part of the theorem (for divergent series). Ulisse Dini proved the complete form and a weak form of the second part. Alfred Pringsheim proved the second part of the theorem. The third part is due to Ernesto Cesàro.