Uniformly bounded derivatives implies globally analytic: Difference between revisions
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===Global statement=== | ===Global statement=== | ||
Suppose <math>f</math> is an infinitely differentiable function on <math>\R</math> such that, for any fixed <math>a | Suppose <math>f</math> is an infinitely differentiable function on <math>\R</math> such that, for any fixed <math>a<b \in \R</math>, there is a constant <math>C</math> (possibly dependent on <math>a,b</math>) such that for all nonnegative integers <math>n</math>, we have: | ||
<math>|f^{(n)}( | <math>|f^{(n)}(t)| \le C \ \forall t \in [a,b]</math> | ||
Then, <math>f</math> is a [[globally analytic function]]: the [[Taylor series]] of <math>f</math> about any point in <math>\R</math> converges to <math>f</math>. In particular, the Taylor series of <math>f</math> about 0 converges to <math>f</math>. | Then, <math>f</math> is a [[globally analytic function]]: the [[Taylor series]] of <math>f</math> about any point in <math>\R</math> converges to <math>f</math>. In particular, the Taylor series of <math>f</math> about 0 converges to <math>f</math>. | ||
==Facts used== | |||
# [[uses::Max-estimate version of Lagrange formula]] | |||
==Examples== | ==Examples== | ||
The functions <math>\exp, \sin, \cos</math> all fit this description. | The functions <math>\exp, \sin, \cos</math> all fit this description. | ||
If <math>f = \exp</math>, we know that each of the derivatives equals <math>\exp</math>, so <math>f^{(n)}(t) = f(t)</math> for all <math>t \in [a,b]</math>. Since <math>\exp</math> is continuous, it is bounded on the closed interval <math>[a,b]</math>, and the upper bound for <math>\exp</math> thus serves as a uniform bound for all its derivatives. (In fact, since <math>f</math> is increasing, we can explicitly take <math>C = \exp(b)</math>). | |||
For <math>f = \sin</math> or <math>f = \cos</math>, we know that all the derivatives are <math>\pm \sin</math> or <math>\pm \cos</math>, so their magnitude is at most 1. Thus, we can take <math>C = 1</math>. | |||
==Proof== | |||
'''Given''': <math>f</math> is an infinitely differentiable function on <math>\R</math> such that, for any fixed <math>a,b \in \R</math>, there is a constant <math>C</math> (possibly dependent on <math>a,b</math>) such that for all nonnegative integers <math>n</math>, we have: | |||
<math>|f^{(n)}(t)| \le C \ \forall t \in [a,b]</math> | |||
A point <math>x_0 \in \R</math> and a point <math>x \in \R</math>. | |||
'''To prove''': The Taylor series of <math>f</math> at <math>x_0</math>, evaluated at <math>x</math>, converges to <math>f(x)</math>. | |||
'''Proof''': Note that if <math>x_0 = x</math>, there is nothing to prove, so we consider the case <math>x \ne x_0</math>. | |||
In order to show this, it suffices to show that <math>\lim_{n \to \infty} P_n(f;x_0)(x) = f(x)</math> where <math>P_n(f;x_0)(x)</math> denotes the <math>n^{th}</math> Taylor polynomial of <math>f</math> at <math>x_0</math>, evaluated at <math>x</math>. | |||
This in turn is equivalent to showing that the ''remainder'' approaches zero: | |||
''''Want to show''': <math>\lim_{n \to \infty} R_n(f;x_0)(x) = 0</math> | |||
where <math>R_n(f;x_0)(x) = f(x) - P_n(f;x_0)(x)</math>. | |||
'''Proof of what we want to show''': By Fact (1), we have that: | |||
<math>|R_n(f;x_0)(x)| \le \left(\max_{t \in J} |f^{(n+1)}(t)|\right) \frac{|x - x_0|^{n+1}}{(n + 1)!}</math> | |||
where <math>J</math> is the interval joining <math>x_0</math> to <math>x</math>. Let <math>a = \min \{ x,x_0 \}</math> and <math>b = \max \{ x, x_0 \}</math>. The interval <math>J</math> is the interval <math>[a,b]</math>. | |||
Now, from the given data, there exists <math>C</math>, dependent on <math>x</math> and <math>x_0</math> but ''not'' on <math>n</math>, such that: | |||
<math>\max_{t \in J} |f^{(n+1)}(t)| \le C \ \forall \ n</math> | |||
Plugging this in, we get that: | |||
<math>|R_n(f;x_0)(x)| \le C \frac{|x - x_0|^{n+1}}{(n + 1)!}</math> | |||
Now taking the limit as <math>n \to \infty</math>, we get: | |||
<math>\lim_{n \to \infty} |R_n(f;x_0)(x)| \le C \lim_{n \to \infty} \frac{|x - x_0|^{n+1}}{(n + 1)!}</math> | |||
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. | |||
Latest revision as of 20:27, 12 July 2012
Statement
Global statement
Suppose is an infinitely differentiable function on such that, for any fixed , there is a constant (possibly dependent on ) such that for all nonnegative integers , we have:
Then, is a globally analytic function: the Taylor series of about any point in converges to . In particular, the Taylor series of about 0 converges to .
Facts used
Examples
The functions all fit this description.
If , we know that each of the derivatives equals , so for all . Since is continuous, it is bounded on the closed interval , and the upper bound for thus serves as a uniform bound for all its derivatives. (In fact, since is increasing, we can explicitly take ).
For or , we know that all the derivatives are or , so their magnitude is at most 1. Thus, we can take .
Proof
Given: is an infinitely differentiable function on such that, for any fixed , there is a constant (possibly dependent on ) such that for all nonnegative integers , we have:
A point and a point .
To prove: The Taylor series of at , evaluated at , converges to .
Proof: Note that if , there is nothing to prove, so we consider the case .
In order to show this, it suffices to show that where denotes the Taylor polynomial of at , evaluated at .
This in turn is equivalent to showing that the remainder approaches zero:
'Want to show:
where .
Proof of what we want to show: By Fact (1), we have that:
where is the interval joining to . Let and . The interval is the interval .
Now, from the given data, there exists , dependent on and but not on , such that:
Plugging this in, we get that:
Now taking the limit as , we get:
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.