In mathematics, the Riemann series theorem, also called the Riemann rearrangement theorem, named after 19th-century German mathematician Bernhard Riemann, says that if an infinite series of real numbers is conditionally convergent, then its terms can be arranged in a permutation so that the new series converges to an arbitrary real number, or diverges. This implies that a series of real numbers is absolutely convergent if and only if it is unconditionally convergent.
As an example, the series
1-1+ | 1 | - |
2 |
1 | + | |
2 |
1 | - | |
3 |
1 | + | |
3 |
1 | - | |
4 |
1 | |
4 |
+...
converges to 0 (for a sufficiently large number of terms, the partial sum gets arbitrarily near to 0); but replacing all terms with their absolute values gives
1+1+
1 | |
2 |
+
1 | |
2 |
+
1 | |
3 |
+
1 | |
3 |
+...
which sums to infinity. Thus, the original series is conditionally convergent, and can be rearranged (by taking the first two positive terms followed by the first negative term, followed by the next two positive terms and then the next negative term, etc.) to give a series that converges to a different sum, such as
1+ | 1 | - |
2 |
1 | + | |
3 |
1 | - | |
4 |
1 | |
2 |
+...
which evaluates to ln 2. More generally, using this procedure with p positives followed by q negatives gives the sum ln(p/q). Other rearrangements give other finite sums or do not converge to any sum.
It is a basic result that the sum of finitely many numbers does not depend on the order in which they are added. For example, . The observation that the sum of an infinite sequence of numbers can depend on the ordering of the summands is commonly attributed to Augustin-Louis Cauchy in 1833. He analyzed the alternating harmonic series, showing that certain rearrangements of its summands result in different limits. Around the same time, Peter Gustav Lejeune Dirichlet highlighted that such phenomena are ruled out in the context of absolute convergence, and gave further examples of Cauchy's phenomenon for some other series which fail to be absolutely convergent.
In the course of his analysis of Fourier series and the theory of Riemann integration, Bernhard Riemann gave a full characterization of the rearrangement phenomena. He proved that in the case of a convergent series which does not converge absolutely (known as conditional convergence), rearrangements can be found so that the new series converges to any arbitrarily prescribed real number. Riemann's theorem is now considered as a basic part of the field of mathematical analysis.
For any series, one may consider the set of all possible sums, corresponding to all possible rearrangements of the summands. Riemann’s theorem can be formulated as saying that, for a series of real numbers, this set is either empty, a single point (in the case of absolute convergence), or the entire real number line (in the case of conditional convergence). In this formulation, Riemann’s theorem was extended by Paul Lévy and Ernst Steinitz to series whose summands are complex numbers or, even more generally, elements of a finite-dimensional real vector space. They proved that the set of possible sums forms a real affine subspace. Extensions of the Lévy–Steinitz theorem to series in infinite-dimensional spaces have been considered by a number of authors.
A series converges if there exists a value
\ell
(S1,S2,S3,\ldots), Sn=
n | |
\sum | |
k=1 |
ak,
converges to
\ell
\left\vertSn-\ell\right\vert\le\varepsilon.
A series converges conditionally if the series converges but the series diverges.
A permutation is simply a bijection from the set of positive integers to itself. This means that if
\sigma
b,
a
\sigma(a)=b.
x\ney
\sigma(x)\ne\sigma(y)
Suppose that
(a1,a2,a3,\ldots)
M
\sigma
infty | |
\sum | |
n=1 |
a\sigma=M.
There also exists a permutation
\sigma
infty | |
\sum | |
n=1 |
a\sigma=infty.
The sum can also be rearranged to diverge to
-infty
The alternating harmonic series is a classic example of a conditionally convergent series:is convergent, whereasis the ordinary harmonic series, which diverges. Although in standard presentation the alternating harmonic series converges to, its terms can be arranged to converge to any number, or even to diverge.
One instance of this is as follows. Begin with the series written in the usual order,
ln(2)=1-
1 | |
2 |
+
1 | |
3 |
-
1 | |
4 |
+
1 | |
5 |
-
1 | |
6 |
+
1 | |
7 |
-
1 | |
8 |
+
1 | |
9 |
…
and rearrange and regroup the terms as:
\begin{align} &1-
1 | |
2 |
-
1 | |
4 |
+
1 | |
3 |
-
1 | |
6 |
-
1 | |
8 |
+
1 | |
5 |
-
1 | |
10 |
-
1 | |
12 |
+ … \\ =&{}\left(1-
1 | |
2 |
\right)-
1 | |
4 |
+\left(
1 | |
3 |
-
1 | |
6 |
\right)-
1 | |
8 |
+\left(
1 | |
5 |
-
1 | |
10 |
\right)-
1 | |
12 |
+ … \end{align}
where the pattern is: the first two terms are 1 and −1/2, whose sum is 1/2. The next term is −1/4. The next two terms are 1/3 and −1/6, whose sum is 1/6. The next term is −1/8. The next two terms are 1/5 and −1/10, whose sum is 1/10. In general, since every odd integer occurs once positively and every even integers occur once negatively (half of them as multiples of 4, the other half as twice odd integers), the sum is composed of blocks of three which can be simplified as:
\left(
1 | |
2k-1 |
-
1 | |
2(2k-1) |
\right)-
1 | |
4k |
=\left(
1 | |
2(2k-1) |
\right)-
1 | |
4k |
, k=1,2,....
Hence, the above series can in fact be written as:
\begin{align} & | 1 |
2 |
-
1 | |
4 |
+
1 | |
6 |
-
1 | |
8 |
+
1 | |
10 |
+ … +
1 | |
2(2k-1) |
-
1 | |
2(2k) |
+ … \\ ={}&
1 | |
2 |
\left(1-
1 | |
2 |
+
1 | |
3 |
- … \right)=
1 | |
2 |
ln(2) \end{align}
which is half the sum originally, and can only equate to the original sequence if the value were zero. This series can be demonstrated to be greater than zero by the proof of Leibniz's theorem using that the second partial sum is half. Alternatively, the value of
ln(2)
It is true that the sequence:
\{bn\}=1,-
1 | ,- | |
2 |
1 | , | |
4 |
1 | |
3 |
,-
1 | |
6 |
,-
1 | , | |
8 |
1 | |
5 |
,-
1 | |
10 |
,-
1 | , | |
12 |
1 | |
7 |
,-
1 | ,- | |
14 |
1 | |
16 |
, …
contains all elements in the sequence:
\{an\}=1,-
1 | , | |
2 |
1 | |
3 |
,-
1 | , | |
4 |
1 | |
5 |
,-
1 | , | |
6 |
1 | |
7 |
,-
1 | , | |
8 |
1 | |
9 |
,-
1 | , | |
10 |
1 | |
11 |
,-
1 | , | |
12 |
1 | |
13 |
,-
1 | , | |
14 |
1 | |
15 |
, …
However, since the summation is defined as
infty | |
\sum | |
n=1 |
an:=\limn\to\left(a1+a2+ … +an\right)
infty | |
\sum | |
n=1 |
bn:=\limn\to\left(b1+b2+ … +bn\right)
An efficient way to recover and generalize the result of the previous section is to use the fact that
1+{1\over2}+{1\over3}+ … +{1\overn}=\gamma+lnn+o(1),
where γ is the Euler–Mascheroni constant, and where the notation o(1) denotes a quantity that depends upon the current variable (here, the variable is n) in such a way that this quantity goes to 0 when the variable tends to infinity.
It follows that the sum of q even terms satisfies
{1\over2}+{1\over4}+{1\over6}+ … +{1\over2q}={1\over2}\gamma+{1\over2}lnq+o(1),
and by taking the difference, one sees that the sum of p odd terms satisfies
{1}+{1\over3}+{1\over5}+ … +{1\over2p-1}={1\over2}\gamma+{1\over2}lnp+ln2+o(1).
Suppose that two positive integers a and b are given, and that a rearrangement of the alternating harmonic series is formed by taking, in order, a positive terms from the alternating harmonic series, followed by b negative terms, and repeating this pattern at infinity (the alternating series itself corresponds to, the example in the preceding section corresponds to a = 1, b = 2):
{1}+{1\over3}+ … +{1\over2a-1}-{1\over2}-{1\over4}- … -{1\over2b}+{1\over2a+1}+ … +{1\over4a-1}-{1\over2b+2}- …
Then the partial sum of order (a + b)n of this rearranged series contains positive odd terms and negative even terms, hence
S(a+b)n={1\over2}lnp+ln2-{1\over2}lnq+o(1)={1\over2}ln\left(
ab\right) | |
+ |
ln2+o(1).
It follows that the sum of this rearranged series is[2]
{1\over2}ln\left(
ab\right) | |
+ |
ln2=ln\left(2\sqrt{
ab} | |
\right). |
Suppose now that, more generally, a rearranged series of the alternating harmonic series is organized in such a way that the ratio between the number of positive and negative terms in the partial sum of order n tends to a positive limit r. Then, the sum of such a rearrangement will be
ln\left(2\sqrt{r}\right),
and this explains that any real number x can be obtained as sum of a rearranged series of the alternating harmonic series: it suffices to form a rearrangement for which the limit r is equal .
Riemann's description of the theorem and its proof reads in full:
This can be given more detail as follows. Recall that a conditionally convergent series of real terms has both infinitely many negative terms and infinitely many positive terms. First, define two quantities,
+ | |
a | |
n |
- | |
a | |
n |
+ | |
a | |
n |
=\begin{cases}an&ifan\geq0\ 0&ifan<0,\end{cases}
- | |
a | |
n |
=\begin{cases}0&ifan\geq0\ an&ifan<0.\end{cases}
That is, the series includes all an positive, with all negative terms replaced by zeroes, and the series includes all an negative, with all positive terms replaced by zeroes. Since is conditionally convergent, both the 'positive' and the 'negative' series diverge. Let be any real number. Take just enough of the positive terms
+ | |
a | |
n |
M<
p1 | |
\sum | |
n=1 |
+ | |
a | |
n |
.
This is possible because the partial sums of the
+ | |
a | |
n |
+infty
p1 | |
M>\sum | |
n=1 |
q1 | |
a | |
n=1 |
-. | |
a | |
n |
- | |
a | |
n |
-infty
p2 | |
M<\sum | |
n=1 |
q1 | |
a | |
n=1 |
-, | |
a | |
n |
+,\ldots. | |
a | |
p2+1 |
pi+1-1 | |
\sum | |
n=1 |
+ | |
a | |
n |
qi | |
+\sum | |
n=1 |
-\leq | |
a | |
n |
pi+1 | |
M<\sum | |
n=1 |
+ | |
a | |
n |
qi | |
+\sum | |
n=1 |
-, | |
a | |
n |
pi+1 | |
0<\left(\sum | |
n=1 |
+ | |
a | |
n |
qi | |
+\sum | |
n=1 |
-\right) | |
a | |
n |
-M\leq
+. | |
a | |
pi+1 |
Every entry in the original sequence appears in this new sequence whose partial sums converge to . Those entries of the original sequence which are zero will appear twice in the new sequence (once in the 'positive' sequence and once in the 'negative' sequence), and every second such appearance can be removed, which does not affect the summation in any way. The new sequence is thus a permutation of the original sequence.
Let be a conditionally convergent series. The following is a proof that there exists a rearrangement of this series that tends to
infty
-infty
The above proof of Riemann's original formulation only needs to be modified so that is selected as the smallest integer larger than such that
pi+1 | |
i+1<\sum | |
n=1 |
+ | |
a | |
n |
qi | |
+\sum | |
n=1 |
-, | |
a | |
n |
pi+1 | |
i+1>\sum | |
n=1 |
+ | |
a | |
n |
qi+1 | |
+\sum | |
n=1 |
-. | |
a | |
n |
- | |
a | |
n |
pi+1 | |
\sum | |
n=1 |
+ | |
a | |
n |
qi+1 | |
+\sum | |
n=1 |
- | |
a | |
n |
>i,
The above proof only needs to be modified so that is selected as the smallest integer larger than such that
pi+1 | |
1<\sum | |
n=1 |
+ | |
a | |
n |
qi | |
+\sum | |
n=1 |
-, | |
a | |
n |
pi+1 | |
-1>\sum | |
n=1 |
+ | |
a | |
n |
qi+1 | |
+\sum | |
n=1 |
-. | |
a | |
n |
Given an infinite series
a=(a1,a2,...)
I\subset\N
I
In{\triangle}I'
S(a,I)=S(a,I')
\triangle
I\subsetI'
S(a,I)\subsetS(a,I')
S(a,I)=\left\{\sumn\in\Nan\right\}
I
S(a,\N)=[-infty,+infty]
Sierpiński proved that rearranging only the positive terms one can obtain a series converging to any prescribed value less than or equal to the sum of the original series, but larger values in general can not be attained.[3] [4] [5] That is, let
a
S(a,\{n\in\N:an>0\})
\left[-infty,\sumn\in\Nan\right]
More generally, let
J
\N
S(a,J)=\cupI\inS(a,I)
Let
Jd
I\subset\N
\limn\toinfty
|[0,n]\capI| | |
n |
=0
Jd
\N
Proof sketch: Given
a
I\inJd
\sumn\inan
\sumn\not\inan
\sumn\inan
[-infty,+infty]
Filipów and Szuca proved that other ideals also have this property.[6]
See main article: Lévy–Steinitz theorem. Given a converging series of complex numbers, several cases can occur when considering the set of possible sums for all series obtained by rearranging (permuting) the terms of that series:
More generally, given a converging series of vectors in a finite-dimensional real vector space E, the set of sums of converging rearranged series is an affine subspace of E.
Encyclopedia: 0249268. Beweis des Satzes, dass jede unbegrenzte arithmetische Progression, deren erstes Glied und Differenz ganze Zahlen ohne gemeinschaftlichen Factor sind, unendlich viele Primzahlen enthält. Lejeune Dirichlet. G.. Peter Gustav Lejeune Dirichlet. Werke. Band I. 21.0016.01. Kronecker. L.. Leopold Kronecker. 1889. Berlin. Dietrich Reimer Verlag. 313–342.
Encyclopedia: Riemann. Bernhard. Bernhard Riemann. Collected Papers. Kendrick Press. Baker. Roger. Christenson. Charles. Orde. Henry. On the representation of a function by a trigonometric series. 2004. 0-9740427-2-2. Heber City, UT. Translation of 1892 German edition. 2121437. 1101.01013.