随机高斯向量的单位模引理与正交性定理
预备定理
Markov 不等式
X为非负随机变量, ε>0,μ=E(X),σ2=V(X), 则
P(∣X−μ∣≥ε)≤ε2σ2
Proof:
\begin{aligned}
\sigma^2 &= \int_{-\infty}^{\infty}(x-\mu)^2p(x)\rmd x\\
&\geq \int_{|x-\mu|\geq \varepsilon}(x-\mu)^2p(x)\rmd x\\
&\geq \varepsilon^2 \int_{|x-\mu|\geq \varepsilon}p(x)\rmd x\\
&=\varepsilon^2 P(|x-\mu|\geq\varepsilon)
\end{aligned}
即
P(∣x−μ∣≥ε)≤ε2σ2
Cramér-Chernoff方法
∀λ>0, 有
∣x−μ∣≥ε⟺eλ∣x−μ∣≥eλε
因此有
P(∣x−μ∣≥ε)=P(eλ∣x−μ∣≥eλε)≤e−λaE(eλ∣x−μ∣)⟺P(∣x−μ∣≥ε)≤λ>0mine−λaE(eλ∣x−μ∣)
从而可以求解最优的概率Pmax以及对应的λ0, 这个上界称为Chernoff Bound
Key Concept
随机高斯向量定义为
\calG=\left\{u\in \bbR^n\Big | u\sim \mathcal{N}(0,\frac{1}{n}I_n)\right\}
单位模引理
\forall u\in \calG,\forall \varepsilon \in (0,1), P(|\|u\|^2-1|\geq \varepsilon)\leq 2\exp(-\frac{\varepsilon^2 n}{8})
Proof:
由Cramér-Chernoff方法
P(∣∥u∥2−1∣≥ε)≤λ>0mine−λεE(eλ∣∥u∥2−1∣)
当∥u∥2≥1时:
P(∥u∥2−1≥ε)=P(∥u∥2≥1+ε)≤λ>0mine−λ(ε+1)E(eλ∥u∥2)
\begin{aligned}
\mathbb{E}(e^{\lambda\|u\|^2})&=\mathbb{E} (e^{\lambda \sum u_i ^2})\\
&=\prod_{i=1}^n \mathbb{E}(e^{\lambda u_i^2})\\
&=\prod_{i=1}^n \int_{-\infty}^{\infty}\frac{\sqrt{n}}{\sqrt{2\pi}}\exp (-\frac{nu_i^2}{2})\exp (\lambda u_i^2)\rmd u_i\\
&=\prod_{i=1}^n \int_{-\infty}^{\infty}\frac{1}{\sqrt{2\pi}}\exp\left(-\frac{n-2\lambda}{n}\frac{v_i^2}{2}\right)\rmd v_i\\
&=\left(\sqrt{\frac{n}{n-2\lambda}}\right)^n
\end{aligned}
即
P(∥u∥−1≥ε)≤λ>0mine−λ(ε+1)(n−2λn)2n
取f(λ)=e−λ(ε+1)(n−2λn)2n
\frac{\rmd f(\lambda)}{\rmd \lambda}=e^{-\lambda(\varepsilon+1)}\left[-(\varepsilon +1)\left(\frac{n}{n-2\lambda}\right)^{\frac{n}{2}}+\frac{n}{2}\left(\frac{n}{n-2\lambda}\right)^{\frac{n}{2}-1}\frac{2n}{(n-2\lambda)^2}\right]=0
根λ0=2(ε+1)nε
故
P(∥u∥−1≥ε)≤f(λ0)=e−2nε(1+ε)2n=e2n(ln(1+ε)−ε)
当∥u∥2<1时
P(1−∥u∥2≤ε)≤λ>0mine−λεE(eλ(1−∥u∥2))=λ>0mine−λ(ε−1)E(e−λ∥u∥2)
\begin{aligned}
\mathbb{E}(-\lambda \|u\|^2)&= \mathbb{E}(e^{-\lambda \sum u_i^2})\\
&=\prod_{i=1}^n \mathbb{E}(e^{-\lambda u_i^2})\\
&=\prod_{i=1}^n \int_{-\infty}^{\infty}\frac{\sqrt{n}}{\sqrt{2\pi}}\exp(-\frac{nu_i^2}{2})\exp(-\lambda u_i^2)\rmd u_i\\
&=\prod_{i=1}^n\int_{-\infty}^{\infty}\frac{1}{\sqrt{2\pi}}\exp (-\frac{n+2\lambda}{n}\frac{v_i^2}{2})\rmd v_i\\
&=\left(\frac{n}{n+2\lambda}\right)^\frac{n}{2}
\end{aligned}
即
P(1−∥u∥2≤ε)≤λ>0mine−λ(ε−1)(n+2λn)2n
取λ0=2(1−ε)εn
P(1−∥u∥2≤ε)≤e2εn(1−ε)2n=e2n(ε+ln(1−ε))
即
{P(∥u∥2−1≥ε)≤e2n(ln(1+ε)−ε)P(1−∥u∥2≤ε)≤e2n(ε+ln(1−ε))
考虑
ln1−ε1+ε>2ε
ln(1+ε)−ε<−Cε2
C>ε∈(0,1)max(ε−ln(1+ε)ε2)=1−ln21≃3.26
通常取C=4,则
{P(∥u∥2−1≥ε)≤e−8nε2P(1−∥u∥2≤ε)≤e−8nε2
P(∣∥u∥2−1∣≥ε)≤2e−8nε2
正交性引理
\forall u,v\in \calG, \forall \varepsilon \in(0,1), P(|\left|\geq \varepsilon)\leq 4\exp(-\frac{\varepsilon^2n}{8})
Proof:
u,v∈G, 则 2u+v,2u−v∈G
一方面
P(∣⟨u,v⟩∣≥ε)≤P(2u+v2−1≥ε)+P(1−2u−v2≥ε)≤4exp(−8ε2n)
另一方面
P(−⟨u,v⟩≥ε)≤P(1−2u+v2≥ε)+P(2u−v2−1≥ε)≤4exp(−8ε2n)
综上
P(∣⟨u,v⟩∣≥ε)≤4exp(−8ε2n)
Chernoff Bound
Moment generating function 矩生成函数
随机变量X的矩生成函数定义为
MX(t)=E(etX)=∫01etxdF(x)
Hoeffding lemma
对于随机变量X, a≤X≤b, E[X]=0,∀x,∣f(x)∣<∞, 则
E(eλ(X−μ))≤exp(8λ(b−a)2)