A power series is an infinite polynomial ∑anxn. The Taylor series is the special case where an=f(n)(0)/n!, but power series appear in quant finance in contexts far beyond Taylor approximation:
Moment generating functions (MGFs) and characteristic functions are power series (or their complex analogues) that encode the entire distribution of a random variable. The MGF of a normalN(μ,σ2) is M(t)=eμt+σ2t2/2, which when expanded as a power series in t yields all moments: E[Xn]=M(n)(0).
Generating functions for discrete distributions (probability generating functions, z-transforms) are power series in a formal variable. They are used in credit portfolio models (generating functions for loss distributions), in counting combinatorial structures (lattice models), and in recursive option pricing.
The radius of convergence of a power series tells you the domain where your approximation is valid — when a pricing approximation breaks down, it is often because you have left the radius of convergence.
Definition
A power series centred at a is:
n=0∑∞cn(x−a)n=c0+c1(x−a)+c2(x−a)2+⋯
where {cn} is a sequence of coefficients and x is the variable. When a=0:
n=0∑∞cnxn
A Taylor series is a power series with cn=f(n)(a)/n!. But a power series can be defined abstractly by its coefficients {cn} without reference to any underlying function.
Radius of convergence
Definition
Every power series ∑cnxn has a radius of convergenceR∈[0,∞] such that:
The series converges absolutely for ∣x∣<R.
The series diverges for ∣x∣>R.
At ∣x∣=R, convergence must be checked case by case.
Computing R
Ratio test:R=limn→∞cn+1cn (when the limit exists).
Root test (Hadamard formula):1/R=limsupn→∞∣cn∣1/n.
Finance implication: The approximation ln(1+R)≈R−R2/2 (from the Taylor/power series of ln(1+x)) is valid for ∣R∣<1 — returns less than 100%. For daily equity returns (∣R∣≈0.01), this is extremely safe. For cumulative returns over long horizons or in crises, ∣R∣ can approach or exceed 1, and the approximation fails.
Properties
Term-by-term differentiation and integration
Within the radius of convergence, a power series can be differentiated and integrated term by term:
dxd∑cnxn=∑ncnxn−1,∫∑cnxndx=∑n+1cnxn+1+C
Both resulting series have the same radius of convergenceR.
Finance application: The MGF M(t)=∑n=0∞n!E[Xn]tn can be differentiated term by term to recover moments: M′(0)=E[X], M′′(0)=E[X2], etc. This is valid within the radius of convergence of the MGF — which may be finite (e.g., for heavy-tailed distributions, the MGF may not exist for t>0).
Uniqueness of coefficients
If ∑anxn=∑bnxn for all x in some interval around 0, then an=bn for all n. Power series representations are unique.
This means: if you find the power series of a function by any method (Taylor's formula, algebraic manipulation, differential equation), the coefficients are guaranteed to be the same.
Multiplication and composition
If f(x)=∑anxn and g(x)=∑bnxn both converge for ∣x∣<R, then:
Product (Cauchy product):
f(x)g(x)=n=0∑∞(k=0∑nakbn−k)xn
Compositionf(g(x)) is valid when ∣g(x)∣<Rf (the inner function must stay within the radius of the outer series).
Moment generating functions as power series
Definition and connection
The moment generating function of a random variable X is:
MX(t)=E[etX]=n=0∑∞n!E[Xn]tn
This is a power series in t with coefficients cn=E[Xn]/n!. It converges in a neighbourhood of t=0 if all moments exist and grow slowly enough.
This converges for all t∈R (radius R=∞), reflecting the fact that the normal distribution has finite moments of all orders and light (Gaussian) tails.
When the MGF does not exist
For heavy-tailed distributions, the MGF may have R=0 — it only converges at t=0. For example, the Student's t distribution with ν degrees of freedom has MGF that diverges for all t=0 when ν is small. The characteristic functionφ(t)=E[eitX] (with i=−1) always exists and serves as a replacement — see Fourier Series and Transforms.
Cumulant generating function
The cumulant generating functionK(t)=lnM(t) is also a power series:
K(t)=n=1∑∞n!κntn
where κn are the cumulants: κ1=μ, κ2=σ2, κ3= skewness ×σ3, κ4= excess kurtosis ×σ4.
For the normal distribution, K(t)=μt+σ2t2/2, so κn=0 for n≥3. Non-zero higher cumulants measure departure from normality. In the Edgeworth expansion (a refinement of the CLT), these cumulants appear as correction terms to the Gaussian approximation.
Probability generating functions
For a discrete random variable N taking non-negative integer values:
GN(z)=E[zN]=k=0∑∞P(N=k)zk
This is a power series in z with coefficients pk=P(N=k).
Finance application — credit portfolio losses: In the CreditRisk+ model, the number of defaults N in a portfolio follows a Poisson mixture. The probability generating function of the total loss is:
GL(z)=i∏GLi(z)
where the product is over independent obligors. The coefficients of GL(z) give the loss distribution. This is computed via power series multiplication — exactly the Cauchy product rule.
Analytic continuation
A function defined by a power series on ∣x∣<R may extend to a larger domain via analytic continuation — finding another power series (centred at a different point) that agrees on an overlap region.
Finance application: The Black-Scholes formula, originally derived for S>0, σ>0, T>0, can be extended to edge cases (e.g., T→0, σ→0) by analytic continuation of the underlying power series expressions. Understanding the radius of convergence tells you which limiting cases are well-behaved and which require special treatment.
Common confusions and pitfalls
"A power series converges everywhere or nowhere." No. Most power series have a finite radius of convergence R, converging inside the disk ∣x∣<R and diverging outside. Only special series like ex converge everywhere (R=∞).
"If the MGF doesn't exist, the distribution has no moments." Not necessarily. The MGF can fail to converge (for any t=0) even when all moments exist, if the moments grow too fast. Conversely, some distributions with finite low-order moments but infinite higher-order moments have MGFs that converge on a bounded interval. The characteristic function is the universal alternative.
"The radius of convergence tells you where the function is undefined." Not exactly. 1/(1−x)=∑xn has R=1, and indeed 1/(1−x) has a pole at x=1. But the function is perfectly well-defined for x>1 — the power series just cannot represent it there. The radius detects the nearest singularity in the complex plane, which may not be visible on the real line.
Where this goes next
Power series connect to:
Taylor Series: Taylor series are power series with cn=f(n)(a)/n!. The radius of convergence of the Taylor series determines where the Taylor approximation is valid.
Fourier Series and Transforms: The characteristic function φ(t)=E[eitX] is a "power series with complex argument" and exists even when the MGF does not.
Asymptotic Expansions: When power series converge too slowly or not at all, asymptotic expansions provide useful approximations.
References
Stewart, J. (2008). Single Variable Calculus: Early Transcendentals (6th ed.). Thomson Brooks/Cole. Ch. 11 Sections 11.8-11.9 (Power Series and Representations of Functions as Power Series) for radius of convergence and algebraic manipulation.