UA MATH563 The central limit theorem of mathematical foundations of probability theory 25 The continuity theorem of characteristic functions of random variables

UA MATH563 The central limit theorem of mathematical foundations of probability theory 25 The continuity theorem of characteristic functions of random variables

Continuity Theorem
assumes {μ n}, μ \{\mu_n\},\mu{ μn},μ is the probability measure,{ϕ n}, ϕ \{\phi_n\},\phi{ fn},ϕ is their characteristic function:

  1. μ n ⇒ μ \ mu_n \ Rightarrow \ mu μnμ, 则ϕ n → ϕ \ phi_n \ to \ phiϕnϕ
  2. ϕ n → ψ \ phi_n \ to \ psi ϕnψ andψ \psiψ is continuous at zero, thenψ \psiψ is the characteristic function, ifμ n ⇒ ν \mu_n \Rightarrow \nuis also knownμnν, 则ψ \ psiψν \ nowCharacteristic function of ν .

Explanation
According to the two conclusions of this theorem, we can get ϕ n → ϕ \phi_n \to \phiϕnϕ等价 于μ n ⇒ μ \ mu_n \ Rightarrow \ muμnμ . There is an interesting condition in the second conclusion,ψ \psiψ is continuous at 0. Why is this condition needed? We can use an example to illustrate that if this condition does not hold, the theorem does not hold:

If X n ∼ N (0, n) X_n \sim N(0,n)XnN(0,n ) , thenX n X_nXnThe density function of will become flatter and flatter, consider the characteristic function
ϕ X n (t) = e − n 2 t 2/2 → ψ (t) = {1, t = 0 0, t ≠ 0 \phi_{X_n}( t) = e^{-n^2t^2/2} \to \psi(t) = \begin{cases} 1, t = 0 \\ 0, t \ne 0 \end{cases}ϕXn(t)=en2 t2/2ψ ( t )={ 1,t=00,t=0

Obviously ψ \psiψ is not continuous at 0. It is not difficult to verify that
μ n (− ∞, x) = ∫ − ∞ x / n 1 2 π e − s 2/2 ds → 1/2 \mu_n(-\infty,x) = \int_{-\infty)^ {x/\sqrt{n}}\frac{1}{\sqrt{2\pi}}e^{-s^2/2}ds \to 1/2μn(,x]=x/n 2 π 1es2/2ds1/2

So obviously X n X_nXnThe limit distribution of does not exist.


Proving the idea The
first conclusion, if μ n ⇒ μ \mu_n \Rightarrow \muμnμ , according to the monotonic convergence theorem,ϕ n → ϕ \phi_n \to \phiϕnF ?

The second conclusion: suppose ϕ n → ψ \phi_n \to \psiϕnψ andψ \psiψ is at0 00 is continuous, andμ n ⇒ ν \mu_n \Rightarrow \nuμnν , the proof is divided into the following steps:

  1. Description {μ n} \{\mu_n\}{ μn} Is tight;
  2. According to the Bolzano-Weierstrass theorem, {μ n} \{\mu_n\}{ μn} 'S sub-column{ϕ nk} \{\phi_{n_k}\}{ fnk} Weak convergence, according to the first conclusion,ϕ nk → ψ \phi_{n_k} \to \psiϕnkψψ \ psiψ is the characteristic function

Here is a proof of Durrett:

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Origin blog.csdn.net/weixin_44207974/article/details/112003862
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