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Conditional convergence
Conditional convergence
from Wikipedia

In mathematics, a series or integral is said to be conditionally convergent if it converges, but it does not converge absolutely.

Definition

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More precisely, a series of real numbers is said to converge conditionally if exists (as a finite real number, i.e. not or ), but

A classic example is the alternating harmonic series given by which converges to , but is not absolutely convergent (see Harmonic series).

Bernhard Riemann proved that a conditionally convergent series may be rearranged to converge to any value at all, including ∞ or −∞; see Riemann series theorem. Agnew's theorem describes rearrangements that preserve convergence for all convergent series.

The Lévy–Steinitz theorem identifies the set of values to which a series of terms in Rn can converge.

Indefinite integrals may also be conditionally convergent. A typical example of a conditionally convergent integral is (see Fresnel integral) where the integrand oscillates between positive and negative values indefinitely, but enclosing smaller areas each time.


See also

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References

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from Grokipedia
In mathematics, conditional convergence refers to the convergence of an infinite series an\sum a_n where the series converges, but the corresponding series of absolute values an\sum |a_n| diverges. This contrasts with absolute convergence, where an\sum |a_n| converges, implying the original series converges regardless of term order or sign changes. A classic example is the alternating harmonic series n=1(1)n+1n\sum_{n=1}^\infty \frac{(-1)^{n+1}}{n}, which converges to ln2\ln 2 by the , but its absolute counterpart n=11n\sum_{n=1}^\infty \frac{1}{n} diverges as the harmonic series. Conditionally convergent series exhibit delicate behavior, as their convergence relies on cancellations between positive and negative terms, making them sensitive to rearrangements. The Riemann rearrangement theorem, proved by in 1852, highlights this fragility: for any conditionally convergent series and any LL, there exists a rearrangement of its terms that converges to LL, or even to ±\pm \infty. This theorem underscores the importance of distinguishing conditional from absolute convergence in , as preserves the sum under permutations, while conditional does not.

Convergence Basics

Absolute Convergence

In , a series n=1an\sum_{n=1}^\infty a_n of real or complex numbers is said to converge absolutely if the series n=1an\sum_{n=1}^\infty |a_n| of the absolute values converges to a finite limit. This condition ensures a stronger form of convergence than ordinary (or conditional) convergence, where the partial sums approach a limit without regard to the signs of the terms. Absolute convergence implies ordinary convergence because, for m > n, |s_m - s_n| = |∑{k=n+1}^m a_k| ≤ ∑{k=n+1}^m |a_k|, and the right-hand side approaches 0 as n, m → ∞ since ∑ |a_n| converges; thus, {s_n} is a and converges to some finite S with |S| ≤ ∑_{n=1}^∞ |a_n|. A key property is that is invariant under permutations of the terms, meaning the sum remains the same regardless of the order in which the terms are added. The concept of was first rigorously defined by in his 1821 work Cours d'analyse, where he distinguished it from ordinary convergence to address issues in series summation. later emphasized its importance in the mid-19th century through his lectures on function theory, highlighting its role in ensuring robust behavior of series under rearrangements and in tests. A classic example is the geometric series n=0rn\sum_{n=0}^\infty r^n for r<1|r| < 1, which converges absolutely because n=0rn=n=0rn\sum_{n=0}^\infty |r|^n = \sum_{n=0}^\infty |r|^n is also a with ratio r<1|r| < 1, summing to 11r\frac{1}{1 - |r|}. In contrast, conditional convergence occurs when an\sum a_n converges but an\sum |a_n| diverges, making the sum sensitive to term order.

Conditional Convergence

In mathematics, particularly in the study of infinite series, conditional convergence describes a scenario where a series converges, but only in a manner dependent on the specific order of its terms. A series n=1an\sum_{n=1}^\infty a_n is said to converge conditionally if the sequence of its partial sums sn=k=1naks_n = \sum_{k=1}^n a_k converges to a finite limit SS, yet the series does not converge absolutely. This contrasts with absolute convergence, where the series n=1an\sum_{n=1}^\infty |a_n| converges, providing a stronger form of convergence that implies ordinary convergence regardless of term arrangement. Formally, n=1an\sum_{n=1}^\infty a_n converges conditionally to SS if limnsn=S\lim_{n \to \infty} s_n = S and limnk=1nak=\lim_{n \to \infty} \sum_{k=1}^n |a_k| = \infty. Here, the failure of absolute convergence serves as the defining prerequisite, as established in standard real analysis texts: every absolutely convergent series is convergent, making conditional convergence the residual case of convergence without this absolute property. A key implication of conditional convergence is its sensitivity to the order of terms; unlike absolutely convergent series, rearrangements of the terms in a conditionally convergent series can yield a different sum or even cause divergence. This order dependence arises precisely because the absolute series diverges, allowing the partial sums to be influenced by how positive and negative terms are interleaved. The distinction from absolute convergence underpins the basic characterization of conditional convergence through a simple proof sketch: since absolute convergence implies convergence via the triangle inequality—specifically, for m>nm > n, smsnk=n+1mak|s_m - s_n| \leq \sum_{k=n+1}^m |a_k|, which approaches 0 as n,mn, m \to \infty if ak\sum |a_k| converges—any convergent series that lacks must be conditionally convergent.

Examples and Illustrations

Alternating Harmonic Series

The alternating harmonic series is defined as the infinite series n=1(1)n+1n=112+1314+.\sum_{n=1}^{\infty} \frac{(-1)^{n+1}}{n} = 1 - \frac{1}{2} + \frac{1}{3} - \frac{1}{4} + \cdots. This series serves as the canonical example of conditional convergence in the context of infinite series. The convergence of the alternating harmonic series follows from the alternating series test, which states that an alternating series (1)n+1bn\sum (-1)^{n+1} b_n with bn>0b_n > 0 converges if the sequence {bn}\{b_n\} is decreasing and limnbn=0\lim_{n \to \infty} b_n = 0. Here, bn=1/nb_n = 1/n, which is positive, decreasing, and approaches 0 as nn \to \infty. The proof relies on showing that the sequence of partial sums is bounded and monotonic in subsequences: the odd-indexed partial sums decrease and are bounded below by 0, while the even-indexed partial sums increase and are bounded above by 1, implying both converge to the same limit by the monotone convergence theorem. The sum of the series equals ln20.693147\ln 2 \approx 0.693147. This result arises as the special case x=1x=1 of the (Taylor expansion of ln(1+x)\ln(1+x)) n=1(1)n+1xnn=ln(1+x)\sum_{n=1}^{\infty} (-1)^{n+1} \frac{x^n}{n} = \ln(1+x) for x<1|x| < 1, extended to x=1x=1 by Abel summation since the series converges at the endpoint of its interval of convergence [1,1][-1, 1]. The series does not converge absolutely because the absolute value series n=11n\sum_{n=1}^{\infty} \frac{1}{n} is the harmonic series, which diverges. The divergence of the harmonic series can be established using the integral test: consider f(x)=1/xf(x) = 1/x, which is positive, continuous, and decreasing on [1,)[1, \infty); the improper integral 11xdx=limblnb=\int_1^{\infty} \frac{1}{x} \, dx = \lim_{b \to \infty} \ln b = \infty diverges, so the series diverges by comparison, as the partial sums exceed the integral from 1 to N+1N+1. Alternatively, it is a pp-series with p=11p=1 \leq 1, which diverges. For approximation, the error when truncating at the nnth partial sum Sn=k=1n(1)k+1kS_n = \sum_{k=1}^n \frac{(-1)^{k+1}}{k} is bounded by the magnitude of the next term: SSn1n+1|S - S_n| \leq \frac{1}{n+1}, with the true sum S=ln2S = \ln 2 lying between SnS_n and Sn+(1)n+1/(n+1)S_n + (-1)^{n+1}/(n+1). An explicit formula for the partial sum is Sn=ln2+(1)n+101xn1+xdx,S_n = \ln 2 + (-1)^{n+1} \int_0^1 \frac{x^n}{1+x} \, dx, where the integral term represents the remainder and alternates in sign while decreasing to 0. Numerical illustration of the partial sums approaching ln20.693147\ln 2 \approx 0.693147 is shown below for the first six terms:
nnPartial Sum SnS_nApproximation Error
11.0000000.306853
20.5000000.193147
30.8333330.140186
40.5833330.109814
50.7833330.090186
60.6166670.076480
The partial sums oscillate around ln2\ln 2, with even sums below and odd sums above, and the amplitude of oscillation diminishes.

Other Standard Examples

Another standard example of a conditionally convergent series is the alternating logarithmic series n=2(1)n+1nlnn\sum_{n=2}^\infty \frac{(-1)^{n+1}}{n \ln n}. This series converges by the alternating series test, as the terms 1nlnn\frac{1}{n \ln n} are positive, decreasing, and approach zero as nn \to \infty. However, the absolute series n=21nlnn\sum_{n=2}^\infty \frac{1}{n \ln n} diverges, which follows from the integral test applied to 2dxxlnx=ln(lnx)2=\int_2^\infty \frac{dx}{x \ln x} = \ln(\ln x) \big|_2^\infty = \infty
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