Uniformly bounded derivatives implies globally analytic

From Calculus

Statement

Global statement

Suppose f is an infinitely differentiable function on R such that, for any fixed a<bR, there is a constant C (possibly dependent on a,b) such that for all nonnegative integers n, we have:

|f(n)(t)|Ct[a,b]

Then, f is a globally analytic function: the Taylor series of f about any point in R converges to f. In particular, the Taylor series of f about 0 converges to f.

Facts used

  1. Max-estimate version of Lagrange formula

Examples

The functions exp,sin,cos all fit this description.

If f=exp, we know that each of the derivatives equals exp, so f(n)(t)=f(t) for all t[a,b]. Since exp is continuous, it is bounded on the closed interval [a,b], and the upper bound for exp thus serves as a uniform bound for all its derivatives. (In fact, since f is increasing, we can explicitly take C=exp(b)).

For f=sin or f=cos, we know that all the derivatives are ±sin or ±cos, so their magnitude is at most 1. Thus, we can take C=1.

Proof

Given: f is an infinitely differentiable function on R such that, for any fixed a,bR, there is a constant C (possibly dependent on a,b) such that for all nonnegative integers n, we have:

|f(n)(t)|Ct[a,b]

A point x0R and a point xR.

To prove: The Taylor series of f at x0, evaluated at x, converges to f(x).

Proof: Note that if x0=x, there is nothing to prove, so we consider the case xx0.

In order to show this, it suffices to show that limnPn(f;x0)(x)=f(x) where Pn(f;x0)(x) denotes the nth Taylor polynomial of f at x0, evaluated at x.

This in turn is equivalent to showing that the remainder approaches zero:

'Want to show: limnRn(f;x0)(x)=0

where Rn(f;x0)(x)=f(x)Pn(f;x0)(x).

Proof of what we want to show: By Fact (1), we have that:

|Rn(f;x0)(x)|(maxtJ|f(n+1)(t)|)|xx0|n+1(n+1)!

where J is the interval joining x0 to x. Let a=min{x,x0} and b=max{x,x0}. The interval J is the interval [a,b].

Now, from the given data, there exists C, dependent on x and x0 but not on n, such that:

maxtJ|f(n+1)(t)|Cn

Plugging this in, we get that:

|Rn(f;x0)(x)|C|xx0|n+1(n+1)!

Now taking the limit as n, we get:

limn|Rn(f;x0)(x)|Climn|xx0|n+1(n+1)!

Since exponentials grow faster than power functions, the expression under the limit goes to zero, so we are left with a right side of zero, hence the left side limit is zero, and we are done.