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泰勒级数,以及光滑 ≠ 解析

把上一篇反过来:若一个函数本身就是幂级数,则它的系数必是其在中心处的导数。这迫使出泰勒级数。但有泰勒级数不等于等于它——著名反例 exp(-1/x^2) 光滑却不解析。

系数被迫等于导数

设 f(x) = sum c_n (x - a)^n 在 a 周围某区间上成立。上一篇我们证明了 f 在那里无穷可微且可逐项微分。反复求导后令 x = a,会消去除一项外的所有项,从而钉死每个系数——这就是系数公式

f(x) = c_0 + c_1 (x-a) + c_2 (x-a)^2 + c_3 (x-a)^3 + ...

Set x = a:                     f(a)   = c_0.
Differentiate once, set x = a: f'(a)  = c_1.
Differentiate twice:           f''(a) = 2 * c_2          -> c_2 = f''(a)/2!
Differentiate k times:         f^(k)(a) = k! * c_k       -> c_k = f^(k)(a)/k!

Hence the ONLY possible coefficients are  c_n = f^(n)(a) / n!.

Consequence (uniqueness): if two power series centered at a agree as
functions near a, they have identical coefficients term by term.
幂级数的系数就是其按比例缩放的导数——别无可能。

有泰勒级数 ≠ 等于它

任何光滑函数都有泰勒级数——只需作 sum f^(n)(a)/n! (x - a)^n。深层问题是该级数是否收敛回 f。在每点的某邻域上等于自身泰勒级数的函数称为实解析的。两者之间的桥梁是泰勒定理:f 在 x 处等于其泰勒级数,当且仅当余项 R_N(x) = f(x) -(第 N 个泰勒多项式)趋于 0。

这确实是不同的条件。令人震惊的事实是:存在光滑函数,其泰勒级数处处收敛,却除中心外处处不等于该函数。这就是光滑但不解析的现象。

标准反例

Define  f(x) = exp(-1/x^2)  for x != 0,  and  f(0) = 0.

Claim 1: f is smooth on all of R, with f^(n)(0) = 0 for EVERY n.

  Near 0 each derivative has the form f^(n)(x) = P(1/x) * exp(-1/x^2),
  where P is a polynomial.  As x -> 0, the substitution t = 1/x^2 -> +inf
  makes  P(1/x) exp(-1/x^2)  behave like  (poly in sqrt(t)) * e^{-t} -> 0,
  because e^{-t} crushes any power of t.  An induction using the
  difference quotient at 0 then shows f^(n)(0) = 0 for all n.

Claim 2: the Maclaurin (Taylor at 0) series of f is
  sum_{n>=0} f^(n)(0)/n! x^n = sum 0 * x^n = 0  (the zero series).

The zero series converges everywhere, with sum 0.
But f(x) = exp(-1/x^2) > 0 for every x != 0.

So f equals its Taylor series ONLY at x = 0, and nowhere else.
f is smooth (C-infinity) but NOT real-analytic at 0.
光滑,泰勒级数处处收敛,却没捕捉到函数的任何信息。