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单词 FormalPowerSeries
释义

formal power series


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Laurent seriesMathworldPlanetmath

Formal power seriesMathworldPlanetmath allow one to employ much of the analyticalmachinery of power seriesMathworldPlanetmath in settings which don’t have natural notionsof convergence. They are also useful in order to compactly describesequencesMathworldPlanetmath and to find closed formulasfor recursively described sequences; this is known as the method ofgenerating functions and will be illustrated below.

We start with a commutative ring R. We want to define the ring offormal power series over R in the variable X, denoted by R[[X]];each element of this ring can be written in a unique way as aninfinite sum of the form n=0anXn, where thecoefficients an are elements of R; any choice of coefficientsan is allowed. R[[X]] is actually a topological ring so thatthese infinite sums are well-defined and convergentMathworldPlanetmathPlanetmath. The additionPlanetmathPlanetmath andmultiplication of such sums follows the usual laws of power series.

Formal construction

Start with the set R of all infiniteMathworldPlanetmathPlanetmath sequences in R.Define addition of two such sequences by

(an)+(bn)=(an+bn)

and multiplication by

(an)(bn)=(k=0nakbn-k).

This turns R into a commutative ring with multiplicativeidentityPlanetmathPlanetmath (1,0,0,…). We identify the element a of R with thesequence (a,0,0,…) and define X:=(0,1,0,0,). Then every elementof R of the form (a0,a1,a2,,aN,0,0,) can be written as the finite sum

n=0NanXn.

In order to extend this equation to infinite series, we need a metricon R. We define d((an),(bn))=2-k, where k is thesmallest natural numberMathworldPlanetmath such that akbk (if there is not suchk, then the two sequences are equal and we define their distance tobe zero). This is a metric which turns R into a topologicalring, and the equation

(an)=n=0anXn

can now be rigorously proven using the notion of convergence arisingfrom d; in fact, any rearrangement of the series convergesPlanetmathPlanetmath to thesame limit.

This topological ring is the ring of formal power series over R andis denoted by R[[X]].

Properties

R[[X]] is an associative algebra over R which contains the ringR[X] of polynomials over R; the polynomials correspond to thesequences which end in zeros.

The geometric series formulaMathworldPlanetmathPlanetmath is valid in R[[X]]:

(1-X)-1=n=0Xn

An element anXn of R[[X]] is invertiblePlanetmathPlanetmath in R[[X]] if and only if itsconstant coefficient a0 is invertible in R (see invertible formal power series).  This implies that theJacobson radicalMathworldPlanetmath of R[[X]] is the ideal generated by X and theJacobson radical of R.

Several algebraicMathworldPlanetmath properties of R are inherited by R[[X]]:

  • if R is a local ringMathworldPlanetmath, then so is R[[X]]

  • if R is NoetherianPlanetmathPlanetmathPlanetmath, then so is R[[X]]

  • if R is an integral domainMathworldPlanetmath, then so is R[[X]]

  • if R is a field, then R[[X]] is a discrete valuation ring.

The metric space (R[[X]],d) is completePlanetmathPlanetmathPlanetmathPlanetmathPlanetmath. The topologyMathworldPlanetmath on R[[X]] isequal to the product topology on R where R is equippedwith the discrete topology. It follows from TychonoffPlanetmathPlanetmath’s theorem thatR[[X]] is compactPlanetmathPlanetmath if and only if R is finite. The topology onR[[X]] can also be seen as the I-adic topology, where I=(X) isthe ideal generated by X (whose elements are precisely the formalpower series with zero constant coefficient).

If R=K is a field, we can consider the quotient field of theintegral domain K[[X]]; it is denoted by K((X)) and called a (formal) power series field. It is atopological field whose elements are called formal Laurentseries; they can be uniquely written in the form

f=n=-ManXn

where M is an integer which depends on the Laurent series f.

Formal power series as functions

In analysisMathworldPlanetmath, every convergent power series defines a function withvalues in the real or complex numbersMathworldPlanetmathPlanetmath. Formal power series can also beinterpreted as functions, but one has to be careful with the domainand codomain. If f=anXn is an element of R[[X]], if S is acommutativePlanetmathPlanetmathPlanetmath associative algebra over R, if I an ideal in S suchthat the I-adic topology on S is complete, and if x is an elementof I, then we can define

f(x):=n=0anxn.

This latter series is guaranteed to converge in S given the aboveassumptionsPlanetmathPlanetmath. Furthermore, we have

(f+g)(x)=f(x)+g(x)

and

(fg)(x)=f(x)g(x)

(unlike in the case of bona fide functions, these formulas are notdefinitions but have to proved).

Since the topology on R[[X]] is the (X)-adic topology and R[[X]]is complete, we can in particular apply power series to other powerseries, provided that the argumentsMathworldPlanetmathPlanetmath don’t have constant coefficients:f(0), f(X2-X) and f((1-X)-1-1) are all well-defined for anyformal power series fR[[X]].

With this formalism, we can give an explicit formula for themultiplicative inverse of a power series f whose constantcoefficient a=f(0) is invertible in R:

f-1=n=0a-n-1(a-f)n

Differentiating formal power series

If f=n=0anXnR[[X]], we define the formal derivative of f as

Df=n=1annXn-1.

This operationMathworldPlanetmath is R-linear, obeys the product ruleMathworldPlanetmath

D(fg)=(Df)g+f(Dg)

and the chain ruleMathworldPlanetmath:

D(f(g))=(Df)(g)Dg

(in case g(0)=0).

In a sense, all formal power series are Taylor seriesMathworldPlanetmath, because iff=anXn, then

(Dkf)(0)=k!ak

(here k! denotes the element 1×(1+1)×(1+1+1)×R.

One can also define differentiationMathworldPlanetmath for formal Laurent series in anatural way, and then the quotient ruleMathworldPlanetmath, in addition to the ruleslisted above, will also be valid.

Power series in several variables

The fastest way to define the ring R[[X1,,Xr]] of formal powerseries over R in r variables starts with the ring S=R[X1,,Xr] of polynomials over R. Let I be the ideal in Sgenerated by X1,,Xr, consider the I-adic topology on S, andform its completion. This results in a complete topological ringcontaining S which is denoted by R[[X1,,Xr]].

For 𝐧=(n1,,nr)r, we write𝐗𝐧=X1n1Xrnr. Then every element ofR[[X1,,Xr]] can be written in a unique was as a sum

𝐧ra𝐧𝐗𝐧

where the sum extends over all 𝐧r. These sums convergefor any choice of the coefficients a𝐧R and the orderin which the summation is carried out does not matter.

If J is the ideal in R[[X1,,Xr]] generated by X1,,Xr(i.e. J consists of those power series with zero constantcoefficient), then the topology on R[[X1,,Xr]] is the J-adictopology.

Since R[[X1]] is a commutative ring, we can define its powerseries ring, say R[[X1]][[X2]]. This ring is naturally isomorphicPlanetmathPlanetmathPlanetmath tothe ring R[[X1,X2]] just defined, but as topological rings the twoare different.

If K=R is a field, then K[[X1,,Xr]] is a unique factorizationdomainMathworldPlanetmath.

Similar to the situation described above, we can “apply” powerseries in several variables to other power series with zero constantcoefficients. It is also possible to define partial derivativesMathworldPlanetmath forformal power series in a straightforward way. Partial derivativescommute, as they do for continuously differentiable functions.

Uses

One can use formal power series to prove several relationsMathworldPlanetmathPlanetmath familarfrom analysis in a purely algebraic setting. Consider for instance thefollowing elements of [[X]]:

sin(X):=n=0(-1)n(2n+1)!X2n+1
cos(X):=n=0(-1)n(2n)!X2n

Then one can easily show that

sin2(X)+cos2(X)=1

and

Dsin=cos

as well as

sin(X+Y)=sin(X)cos(Y)+cos(X)sin(Y)

(the latter being valid in the ring [[X,Y]]).

As an example of the method of generating functions, consider theproblem of finding a closed formula for the Fibonacci numbersMathworldPlanetmath fndefined by fn+2=fn+1+fn, f0=0, and f1=1. We work in thering [[X]] and define the power series

f=n=0fnXn;

f is called the generating function for the sequence (fn).The generating function for the sequence (fn-1) is Xf whilethat for (fn-2) is X2f. From the recurrence relation, wetherefore see that the power series Xf+X2f agrees with f exceptfor the first two coefficients. Taking these into account, we findthat

f=Xf+X2f+X

(this is the crucial step; recurrence relations can almost always betranslated into equations for the generating functions). Solving thisequation for f, we get

f=X1-X-X2.

Using the golden ratioMathworldPlanetmath ϕ1=(1+5)/2 andϕ2=(1-5)/2, we can write the latter expression as

15(11-ϕ1X-11-ϕ2X).

These two power series are known explicitly because they are geometricseries; comparing coefficients, we find the explicit formula

fn=15(ϕ1n-ϕ2n).

In algebra, the ring K[[X1,,Xr]] (where K is a field) is oftenused as the “standard, most general” complete local ring over K.

Universal property

The power series ring R[[X1,,Xr]] can be characterized by thefollowing universal property: if S is a commutative associativealgebra over R, if I is an ideal in S such that the I-adictopology on S is complete, and if x1,,xrI are given, thenthere exists a unique Φ:R[[X1,,Xr]]S with thefollowing properties:

  • Φ is an R-algebra homomorphism

  • Φ is continuousMathworldPlanetmathPlanetmath (http://planetmath.org/Continuous)

  • Φ(Xi)=xi for i=1,,r.

Titleformal power series
Canonical nameFormalPowerSeries
Date of creation2013-03-22 12:49:30
Last modified on2013-03-22 12:49:30
OwnerAxelBoldt (56)
Last modified byAxelBoldt (56)
Numerical id14
AuthorAxelBoldt (56)
Entry typeTopic
Classificationmsc 13H05
Classificationmsc 13B35
Classificationmsc 13J05
Classificationmsc 13F25
Related topicPowerSeries
Related topicSumOfKthPowersOfTheFirstNPositiveIntegers
Related topicPolynomialRingOverIntegralDomain
Related topicFiniteRingHasNoProperOverrings
Definesformal power series
Definesgenerating function
Definesformal Laurent series
Definespower series field
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