Series

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A series is an infinite ordered set of terms combined together by the addition operator. The term "infinite series" is sometimes used to emphasize the fact that series contain an infinite number of terms. The order of the terms in a series can matter, since the Riemann series theorem states that, by a suitable rearrangement of terms, a so-called conditionally convergent series may be made to converge to any desired value, or to diverge.

Conditions for convergence of a series can be determined in the Wolfram Language using SumConvergence[a, n].

If the difference between successive terms of a series is a constant, then the series is said to be an arithmetic series. A series for which the ratio of each two consecutive terms a_(k+1)/a_k is a constant function of the summation index k is called a geometric series. The more general case of the ratio a rational function of k produces a series called a hypergeometric series.

A series may converge to a definite value, or may not, in which case it is called divergent. Let the terms in a series be denoted a_i, let the kth partial sum be given by

 S_k=sum_(i=1)^ka_i,
(1)

and let the sequence of partial sums be given by {S_1=a_1,S_2=a_1+a_2,S_3=a_1+a_2+a_3,...}. If the sequence of partial sums converges to a definite value, the series is said to converge. On the other hand, if the sequence of partial sums does not converge to a limit (e.g., it oscillates or approaches +/-infty), the series is said to diverge. An example of a convergent series is the geometric series

 sum_(n=0)^infty(1/2)^n=2,
(2)

and an example of a divergent series is the harmonic series

 sum_(n=1)^infty1/n=infty.
(3)

Interestingly, while the harmonic series diverges to infinity, the alternating harmonic series converges to the natural logarithm of 2,

 sum_(k=1)^infty((-1)^(k-1))/k=ln2.
(4)

Another well-known convergent infinite series is Brun's constant.

A number of methods known as convergence tests can be used to determine whether a given series converges. Although terms of a series can have either sign, convergence properties can often be computed in the "worst case" of all terms being positive, and then applied to the particular series at hand. A series of terms a_n is said to be absolutely convergent if the series formed by taking the absolute values of the a_n,

 sum_(n)|a_n|,
(5)

converges.

An especially strong type of convergence is called uniform convergence, and series which are uniformly convergent have particularly "nice" properties. For example, the sum of a uniformly convergent series of continuous functions is continuous. A convergent series can be differentiated term by term, provided that the functions of the series have continuous derivatives and that the series of derivatives is uniformly convergent. Finally, a uniformly convergent series of continuous functions can be integrated term by term.

For a table listing the coefficients for various series operations, see Abramowitz and Stegun (1972, p. 15).

While it can be difficult to calculate analytical expressions for arbitrary convergent infinite series, many algorithms can handle a variety of common series types. The Wolfram Language computational system implements many of these algorithms. General techniques also exist for computing the numerical values of any but the most pathological series (Braden 1992).

A particular infinite series identity is given by

sum_(k=1, 3, 5,...)^(infty)(e^(-kx)sin(ky))/k=1/2i[coth^(-1)(e^(x+iy))-coth^(-1)(e^(x-iy))]
(6)
=1/2tan^(-1)((siny)/(sinhx))
(7)

for x>0.

Apostol (1997, p. 25) gives the analytic sum

 sum_(n=1,3,5,...)^infty(n^(4k+1))/(1+e^(npi))=(2^(4k+1)-1)/(8k+4)B_(4k+2),
(8)

where B_k is a Bernoulli number.

Ramanujan found the interesting series identity

 sum_(n=0)^infty(-1)^n((3n)!)/([n!(3n)!]^3)x^(2n) 
 =[sum_(n=0)^infty(x^n)/((n!)^3)][sum_(n=0)^infty(-1)^n(x^n)/((n!)^3)]
(9)

(Preece 1928; Hardy 1999, p. 7), which can be written as the hypergeometric identity

 _2F_7(1/3,2/3;1/2,1/2,1/2,1,1,1,1;-(27)/(64)x^2) 
 =_0F_2(;1,1;x)_0F_2(;1,1;-x).
(10)

Infinite series of the following type (power sums) can also be computed analytically,

(sum_(k=0)^(infty)x^k)^p=(1-x)^(-p)
(11)
=1/((p-1)!)sum_(n=0)^(infty)((n+p-1)!)/(n!)x^n
(12)
=1/((p-1)!)sum_(n=0)^(infty)(n+1)_(p-1)x^n,
(13)

where (n)_p is a Pochhammer symbol.

Gosper noted the sum

sum_(n=1)^(infty)1/(n^2)cos(9/(npi+sqrt(n^2pi^2-9)))=sum_(n=1)^(infty)((-1)^ncos(sqrt(n^2pi^2-9)))/(n^2)
(14)
=-(pi^2)/(12e^3)
(15)
=-0.040948222...
(16)

(OEIS A100074).

An infinite series of the following form can be done in closed form.

 sum_(k=1)^infty1/([1+k^2pi^2]^n)=(P_n(e^2))/(2^n(n-1)!(e^2-1)^n),
(17)

where P_n(e^2) is an nth order polynomial in e^2. The first few polynomials are

P_1=2
(18)
P_2=-e^4+8e^2-3
(19)
P_3=-5e^6+41e^4-31e^2+11
(20)
P_4=-33e^8+286e^6-344e^4+250e^2-63
(21)

(OEIS A085470).

The related infinite series

 sum_(k=1)^infty1/([1+(k+1/2)^2pi^2]^n)=(Q_n(e))/(2^(n+1)n!(e^2+1)^n)-(4^n)/((4+pi^2)^n)
(22)

can also be done in closed form, where Q_n(e^2) is an nth order polynomial in e^2. The first few polynomials are

Q_1=e^2-1
(23)
Q_2=e^4-4e^2-1
(24)
Q_3=3e^6-17e^4-7e^2-3
(25)
Q_4=15e^8-94e^6-56e^4-58e^2-15
(26)
Q_5=105e^(10)-657e^8-578e^6-982e^4-503-105
(27)

(OEIS A085471).

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