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In
mathematics Mathematics is a field of study that discovers and organizes methods, Mathematical theory, theories and theorems that are developed and Mathematical proof, proved for the needs of empirical sciences and mathematics itself. There are many ar ...
, the Riemann series theorem, also called the Riemann rearrangement theorem, named after 19th-century German mathematician
Bernhard Riemann Georg Friedrich Bernhard Riemann (; ; 17September 182620July 1866) was a German mathematician who made profound contributions to analysis, number theory, and differential geometry. In the field of real analysis, he is mostly known for the f ...
, says that if an
infinite series In mathematics, a series is, roughly speaking, an addition of infinitely many terms, one after the other. The study of series is a major part of calculus and its generalization, mathematical analysis. Series are used in most areas of mathemati ...
of real numbers is conditionally convergent, then its terms can be arranged in a
permutation In mathematics, a permutation of a set can mean one of two different things: * an arrangement of its members in a sequence or linear order, or * the act or process of changing the linear order of an ordered set. An example of the first mean ...
so that the new series converges to an arbitrary real number, and rearranged such that the new series diverges. This implies that a series of real numbers is absolutely convergent
if and only if In logic and related fields such as mathematics and philosophy, "if and only if" (often shortened as "iff") is paraphrased by the biconditional, a logical connective between statements. The biconditional is true in two cases, where either bo ...
it is unconditionally convergent. As an example, the series : 1-1+\frac-\frac+\frac-\frac+\frac-\frac+\dots 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 + \frac + \frac + \frac + \frac + \dots 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 + \frac - 1 + \frac+\frac-\frac+\dots 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.


History

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 Baron Augustin-Louis Cauchy ( , , ; ; 21 August 1789 – 23 May 1857) was a French mathematician, engineer, and physicist. He was one of the first to rigorously state and prove the key theorems of calculus (thereby creating real a ...
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 Johann Peter Gustav Lejeune Dirichlet (; ; 13 February 1805 – 5 May 1859) was a German mathematician. In number theory, he proved special cases of Fermat's last theorem and created analytic number theory. In analysis, he advanced the theory o ...
highlighted that such phenomena are ruled out in the context of
absolute convergence In mathematics, an infinite series of numbers is said to converge absolutely (or to be absolutely convergent) if the sum of the absolute values of the summands is finite. More precisely, a real or complex series \textstyle\sum_^\infty a_n is said ...
, 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 A Fourier series () is an Series expansion, expansion of a periodic function into a sum of trigonometric functions. The Fourier series is an example of a trigonometric series. By expressing a function as a sum of sines and cosines, many problems ...
and the theory of Riemann integration,
Bernhard Riemann Georg Friedrich Bernhard Riemann (; ; 17September 182620July 1866) was a German mathematician who made profound contributions to analysis, number theory, and differential geometry. In the field of real analysis, he is mostly known for the f ...
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 In mathematics, a series or integral is said to be conditionally convergent if it converges, but it does not converge absolutely. Definition More precisely, a series of real numbers \sum_^\infty a_n is said to converge conditionally if \lim_\,\s ...
), 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 Analysis is the branch of mathematics dealing with continuous functions, limit (mathematics), limits, and related theories, such as Derivative, differentiation, Integral, integration, measure (mathematics), measure, infinite sequences, series ( ...
. 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 A number line is a graphical representation of a straight line that serves as spatial representation of numbers, usually graduated like a ruler with a particular origin point representing the number zero and evenly spaced marks in either direc ...
(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 number In mathematics, a complex number is an element of a number system that extends the real numbers with a specific element denoted , called the imaginary unit and satisfying the equation i^= -1; every complex number can be expressed in the for ...
s or, even more generally, elements of a finite-dimensional
real vector space Real may refer to: Currencies * Argentine real * Brazilian real (R$) * Central American Republic real * Mexican real * Portuguese real * Spanish real * Spanish colonial real Nature and science * Reality, the state of things as they exist, ...
. They proved that the set of possible sums forms a real
affine subspace In mathematics, an affine space is a geometry, geometric structure (mathematics), structure that generalizes some of the properties of Euclidean spaces in such a way that these are independent of the concepts of distance (mathematics), distance ...
. Extensions of the Lévy–Steinitz theorem to series in infinite-dimensional spaces have been considered by a number of authors.


Definitions

A series \sum_^\infty a_n converges if there exists a value \ell such that the
sequence In mathematics, a sequence is an enumerated collection of objects in which repetitions are allowed and order matters. Like a set, it contains members (also called ''elements'', or ''terms''). The number of elements (possibly infinite) is cal ...
of the partial sums :(S_1, S_2, S_3, \ldots), \quad S_n = \sum_^n a_k, converges to \ell. That is, for any ''ε'' > 0, there exists an integer ''N'' such that if ''n'' ≥ ''N'', then :\left\vert S_n - \ell \right\vert \le \varepsilon. A series converges conditionally if the series \sum_^\infty a_n converges but the series \sum_^\infty \left\vert a_n \right\vert diverges. A permutation is simply a
bijection In mathematics, a bijection, bijective function, or one-to-one correspondence is a function between two sets such that each element of the second set (the codomain) is the image of exactly one element of the first set (the domain). Equival ...
from the
set Set, The Set, SET or SETS may refer to: Science, technology, and mathematics Mathematics *Set (mathematics), a collection of elements *Category of sets, the category whose objects and morphisms are sets and total functions, respectively Electro ...
of
positive integer In mathematics, the natural numbers are the numbers 0, 1, 2, 3, and so on, possibly excluding 0. Some start counting with 0, defining the natural numbers as the non-negative integers , while others start with 1, defining them as the positiv ...
s to itself. This means that if \sigma is a permutation, then for any positive integer b, there exists exactly one positive integer a such that \sigma (a) = b. In particular, if x \ne y, then \sigma (x) \ne \sigma (y).


Statement of the theorem

Suppose that (a_1, a_2, a_3, \ldots) is a sequence of
real number In mathematics, a real number is a number that can be used to measure a continuous one- dimensional quantity such as a duration or temperature. Here, ''continuous'' means that pairs of values can have arbitrarily small differences. Every re ...
s, and that \sum_^\infty a_n is conditionally convergent. Let M be a real number. Then there exists a
permutation In mathematics, a permutation of a set can mean one of two different things: * an arrangement of its members in a sequence or linear order, or * the act or process of changing the linear order of an ordered set. An example of the first mean ...
\sigma such that :\sum_^\infty a_ = M. There also exists a permutation \sigma such that :\sum_^\infty a_ = \infty. The sum can also be rearranged to diverge to -\infty or to fail to approach any limit, finite or infinite.


Alternating harmonic series


Changing the sum

The alternating harmonic series is a classic example of a conditionally convergent series:\sum_^\infty \fracis convergent, whereas\sum_^\infty \left, \frac \ = \sum_^\infty \fracis 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 - \frac + \frac - \frac + \frac - \frac + \frac - \frac + \frac\cdots, and rearrange and regroup the terms as \begin & 1 - \frac - \frac + \frac - \frac - \frac + \frac - \frac - \frac + \cdots\\ =& \left( 1 - \frac \right) - \frac + \left(\frac - \frac\right) - \frac + \left(\frac - \frac\right) - \frac + \cdots, \end 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, each of which can be simplified as \left( \frac - \frac \right)- \frac = \left(\frac\right)- \frac,\quad k = 1, 2, \dots. Hence, the above series can in fact be written as \begin &\frac - \frac + \frac - \frac + \frac + \cdots + \frac - \frac + \cdots \\ =& \frac\left(1 - \frac + \frac - \cdots\right) = \frac \ln(2), \end 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) which it converges to, cannot be zero. Hence, the value of the sequence is shown to depend on the order in which series is computed. It is true that the sequence \=1, -\frac,-\frac,\frac, -\frac, -\frac,\frac, -\frac, -\frac,\frac, -\frac,-\frac,\cdots contains all elements in the sequence \=1, -\frac,\frac, -\frac,\frac, -\frac,\frac, -\frac,\frac, -\frac,\frac, -\frac,\frac, -\frac,\frac,\cdots. However, since the summation is defined as \sum^_a_n:=\lim_ \left(a_1 + a_2 + \cdots + a_n\right) and \sum^_b_n:=\lim_ \left(b_1 + b_2 + \cdots + b_n\right), the order of the terms can influence the limit.


Getting an arbitrary sum

An efficient way to recover and generalize the result of the previous section is to use the fact that :1 + + + \cdots + = \gamma + \ln n + o(1), where ''γ'' is the
Euler–Mascheroni constant Euler's constant (sometimes called the Euler–Mascheroni constant) is a mathematical constant, usually denoted by the lowercase Greek letter gamma (), defined as the limiting difference between the harmonic series and the natural logarith ...
, 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 : + + + \cdots + = \, \gamma + \ln q + o(1), and by taking the difference, one sees that the sum of ''p'' odd terms satisfies : + + + \cdots + = \, \gamma + \ln p + \ln 2 + 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): : + + \cdots + - - - \cdots - + + \cdots + - - \cdots Then the partial sum of order (''a'' + ''b'')''n'' of this rearranged series contains positive odd terms and negative even terms, hence :S_ = \ln p + \ln 2 - \ln q + o(1) = \ln\left(\frac ab\right) + \ln 2 + o(1). It follows that the sum of this rearranged series is : \ln\left(\frac ab\right) + \ln 2 = \ln\left( 2 \sqrt \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 \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 .


Proof


Existence of a rearrangement that sums to any positive real ''M''

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_^ and a_^ by: :a_^ = \begina_n&\texta_n\geq 0\\ 0&\texta_n<0,\end \qquad a_^ = \begin0&\texta_n\geq 0\\ a_n&\texta_n<0.\end That is, the series \sum_^\infty a_n^ includes all ''a''''n'' positive, with all negative terms replaced by zeroes, and the series \sum_^\infty a_n^ includes all ''a''''n'' negative, with all positive terms replaced by zeroes. Since \sum_^\infty a_n is conditionally convergent, both the 'positive' and the 'negative' series diverge. Let be any real number. Take just enough of the positive terms a_^ so that their sum exceeds . That is, let be the smallest positive integer such that :M < \sum_^ a_^. This is possible because the partial sums of the a_^ series tend to +\infty. Now let be the smallest positive integer such that :M>\sum_^ a_n^++\sum_^ a_n^-. This number exists because the partial sums of a_^ tend to -\infty. Now continue inductively, defining as the smallest integer larger than such that :M<\sum_^a_n^++\sum_^a_n^-, and so on. The result may be viewed as a new sequence :a_1^+,\ldots,a_^+,a_1^-,\ldots,a_^-,a_^+,\ldots,a_^+,a_^-,\ldots,a_^-,a_^+,\ldots. Furthermore, the partial sums of this new sequence converge to . This can be seen from the fact that for any , :\sum_^ a_n^+ +\sum_^a_n^-\leq M<\sum_^a_n^+ +\sum_^a_n^-, with the first inequality holding due to the fact that has been defined as the ''smallest'' number larger than which makes the second inequality true; as a consequence, it holds that :0<\left(\sum_^a_n^+ +\sum_^a_n^-\right) - M \leq a_^+. Since the right-hand side converges to zero due to the assumption of conditional convergence, this shows that the 'th partial sum of the new sequence converges to as increases. Similarly, the 'th partial sum also converges to . Since the 'th, 'th, ... 'th partial sums are valued between the 'th and 'th partial sums, it follows that the whole sequence of partial sums converges to . 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.


Existence of a rearrangement that diverges to infinity

Let \sum_^\infty a_i be a conditionally convergent series. The following is a proof that there exists a rearrangement of this series that tends to \infty (a similar argument can be used to show that -\infty can also be attained). 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 :i+1<\sum_^a_n^+ +\sum_^a_n^-, and with selected as the smallest integer larger than such that :i+1>\sum_^a_n^+ +\sum_^a_n^-. The choice of on the left-hand sides is immaterial, as it could be replaced by any sequence increasing to infinity. Since a_n^- converges to zero as increases, for sufficiently large there is :\sum_^a_n^+ +\sum_^a_n^- > i, and this proves (just as with the analysis of convergence above) that the sequence of partial sums of the new sequence diverge to infinity.


Existence of a rearrangement that fails to approach any limit, finite or infinite

The above proof only needs to be modified so that is selected as the smallest integer larger than such that :1<\sum_^a_n^+ +\sum_^a_n^-, and with selected as the smallest integer larger than such that :-1>\sum_^a_n^+ +\sum_^a_n^-. This directly shows that the sequence of partial sums contains infinitely many entries which are larger than 1, and also infinitely many entries which are less than , so that the sequence of partial sums cannot converge.


Generalizations


Sierpiński theorem

Given an infinite series a = (a_1, a_2, ...), we may consider a set of "fixed points" I \subset \N, and study the real numbers that the series can sum to if we are only allowed to permute indices in I. That is, we letS(a, I) = \left\With this notation, we have: * If I \mathbin I' is finite, then S(a, I) = S(a, I'). Here \triangle means
symmetric difference In mathematics, the symmetric difference of two sets, also known as the disjunctive union and set sum, is the set of elements which are in either of the sets, but not in their intersection. For example, the symmetric difference of the sets \ and ...
. * If I \subset I' then S(a, I) \subset S(a, I'). * If the series is an absolutely convergent sum, then S(a, I) = \left\ for any I. * If the series is a conditionally convergent sum, then by Riemann series theorem, S(a, \N) = \infty, +\infty/math>. 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. That is, let a be a conditionally convergent sum, then S(a, \) contains \left \infty, \sum_ a_n\right/math>, but there is no guarantee that it contains any other number. More generally, let J be an ideal of \N, then we can define S(a, J) = \cup_ S(a, I). Let J_d be the set of all asymptotic density zero sets I\subset \N, that is, \lim_\frac = 0. It's clear that J_d is an ideal of \N. Proof sketch: Given a, a conditionally convergent sum, construct some I\in J_d such that \sum_a_n and \sum_a_n are both conditionally convergent. Then, rearranging \sum_a_n suffices to converge to any number in \infty, +\infty/math>. Filipów and Szuca proved that other ideals also have this property.


Steinitz's theorem

Given a converging series \sum a_nof
complex number In mathematics, a complex number is an element of a number system that extends the real numbers with a specific element denoted , called the imaginary unit and satisfying the equation i^= -1; every complex number can be expressed in the for ...
s, several cases can occur when considering the set of possible sums for all series \sum a_ obtained by rearranging (permuting) the terms of that series: * the series \sum a_n may converge unconditionally; then, all rearranged series converge, and have the same sum: the set of sums of the rearranged series reduces to one point; * the series \sum a_n may fail to converge unconditionally; if ''S'' denotes the set of sums of those rearranged series that converge, then, either the set ''S'' is a line ''L'' in the complex plane C, of the form L = \, \quad a, b \in \Complex, \ b \ne 0, or the set ''S'' is the whole complex plane C. More generally, given a converging series of vectors in a finite-dimensional real
vector space In mathematics and physics, a vector space (also called a linear space) is a set (mathematics), set whose elements, often called vector (mathematics and physics), ''vectors'', can be added together and multiplied ("scaled") by numbers called sc ...
''E'', the set of sums of converging rearranged series is an
affine subspace In mathematics, an affine space is a geometry, geometric structure (mathematics), structure that generalizes some of the properties of Euclidean spaces in such a way that these are independent of the concepts of distance (mathematics), distance ...
of ''E''.


See also

* * Agnew's theorem — describes all rearrangements that preserve convergence to the same sum for all convergent series


References

* * * * * * * * * *


External links

* {{Bernhard Riemann Series (mathematics) Theorems in real analysis Permutations Summability theory Bernhard Riemann