We prove the Central Limit Theorem using characteristic functions (Fourier transforms), the standard approach in modern probability theory.
Proof
Theorem (CLT): Let X1,X2,… be i.i.d. with E[Xi]=0, Var(Xi)=σ2>0. Then Sn=σnX1+⋯+XndN(0,1).
Step 1: Characteristic functions.
The characteristic function of a random variable X is φX(t)=E[eitX]. By Levy's continuity theorem, XndX if and only if φXn(t)→φX(t) pointwise for all t∈R.
The characteristic function of N(0,1) is φZ(t)=e−t2/2.
Step 2: Compute the characteristic function of Sn.
Let Yi=Xi/(σn), so Sn=Y1+⋯+Yn. By independence:
φSn(t)=∏i=1nφYi(t)=[φY1(t)]n=[φX1(σnt)]n
Step 3: Taylor expansion of the characteristic function.
Since E[X1]=0 and E[X12]=σ2, the characteristic function of X1 has the expansion:
φX1(s)=E[eisX1]=1+is⋅E[X1]+2(is)2E[X12]+o(s2)=1−2σ2s2+o(s2)as s→0
Using the fundamental limit limn→∞(1+an/n)n=ea when an→a:
limn→∞φSn(t)=e−t2/2
More rigorously: write φX1(t/σn)=1+wn where wn=−t2/(2n)+o(1/n). Then log(1+wn)=wn+O(wn2)=−t2/(2n)+o(1/n), so nlog(1+wn)→−t2/2, giving φSn(t)=enlog(1+wn)→e−t2/2.
Step 5: Apply Levy's continuity theorem.
Since φSn(t)→e−t2/2=φZ(t) pointwise and e−t2/2 is continuous at t=0, Levy's continuity theorem guarantees SndZ∼N(0,1). □
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RemarkWhy characteristic functions?
The proof via characteristic functions is elegant because: (1) the characteristic function of a sum of independent variables is the product of their characteristic functions, converting convolution to multiplication; (2) pointwise convergence of characteristic functions is equivalent to convergence in distribution (Levy's theorem); (3) the Taylor expansion naturally produces the Gaussian e−t2/2.