Lecture 16 — Gaussian Tail Bounds and Independence

This lecture has two main components:

  • Tail bounds for random variables (Markov, Chebyshev, Chernoff/Exponential tail for the Gaussian).
  • Independence of σ-algebras and random variables via the π–λ theorem.

1. Gaussian Tail Bounds

Let $Z \sim N(0,1)$.

1.1 Exact integral representation

\[P(Z > x) = \int_x^{\infty} \frac{1}{\sqrt{2\pi}} e^{-y^2/2}\, dy, \qquad x>0.\]

The handwritten notes (page 1) perform a change of variable:

  • Let $y = x + z$, so $dy = dz$.
  • Then: \(\int_x^\infty e^{-y^2/2}\,dy = e^{-x^2/2} \int_0^\infty e^{-xz} e^{-z^2/2}\,dz \le e^{-x^2/2} \int_0^\infty e^{-xz}\,dz = e^{-x^2/2} \cdot \frac{1}{x}.\)

Thus:

\[P(Z > x) \le \frac{1}{\sqrt{2\pi}}\frac{e^{-x^2/2}}{x}.\]

1.2 Lower bound

On page 1, the lecture notes show the inequality:

\[\int_x^\infty e^{-y^2/2}\,dy \ge \int_x^\infty \left(1 - \frac{3}{y^4}\right)e^{-y^2/2}\,dy = \left( \frac{1}{x} - \frac{1}{x^3} \right) e^{-x^2/2}.\]

So overall:

\[\boxed{ \left(\frac{1}{x} - \frac{1}{x^3}\right) \frac{e^{-x^2/2}}{\sqrt{2\pi}} \;\le\; P(Z>x) \;\le\; \frac{1}{x} \frac{e^{-x^2/2}}{\sqrt{2\pi}}. }\]

These are the classical Mills ratio bounds.


2. Markov and Chebyshev Inequalities

For any nonnegative $X$,

\[P(X > a) \le \frac{\mathbb{E}[X]}{a}.\]

For any square-integrable $X$ with mean $m$ and variance $\sigma^2$,

\[P(\vert X - m\vert > a) \le \frac{\sigma^2}{a^2}.\]

The handwritten notes then consider shifting to optimize:

Given $Y$ with $\mathbb{E}[Y]=m$, $\operatorname{Var}(Y)=\sigma^2$, the notes derive:

\[P(Y > a) \le P(\vert Y+b\vert > a+b) \le \frac{\mathbb{E}[(Y+b)^2]}{(a+b)^2} = \frac{\sigma^2 + b^2}{(a+b)^2}.\]

Choose $b$ to minimize the right-hand side.
The notes compute:

\[\min_b\ \frac{\sigma^2 + b^2}{(a+b)^2} = \frac{\sigma^2}{\sigma^2 + a^2}.\]

Thus:

\[\boxed{ P(Y > a) \le \frac{\sigma^2}{\sigma^2 + a^2}. }\]

(The algebra is written step-by-step on page 1 of the handwritten notes.)


3. Independence (Durrett Ch. 2.1)

Let $ {\mathcal{F}\alpha}{\alpha\in I} \text{ be sub-σ-algebras of } \mathcal{F}$.

3.1 Definition

They are independent if for all finite choices $\alpha_1,\dots,\alpha_n$ and events $A_i \in \mathcal{F}_{\alpha_i}$,

\[P(A_1 \cap \cdots \cap A_n) = P(A_1)\cdots P(A_n).\]

3.2 Independence of random variables

A family of random variables ${X_\alpha}$ is independent if
${\sigma(X_\alpha)}$ are independent as σ-algebras.

Measurability of $X_\alpha$

Each $X_\alpha: \Omega\to\mathbb{R}$ is $\mathcal{F}/\mathcal{B}(\mathbb{R})$-measurable.

So:

\[\sigma(X_\alpha) = \{ X_\alpha^{-1}(B): B\in\mathcal{B}(\mathbb{R})\}.\]

4. Independence via π–λ Theorem (Key Theorem)

Theorem.
If the collections ${A_i}$ are independent on a π-system and each $A_i$ generates a σ-algebra, then the σ-algebras they generate are independent.

Outline of proof as in notes

Fix an index $1$. Define:

\[\mathcal{L} = \{A\in\mathcal{F} : P(A \cap A_2 \cap\cdots\cap A_n) = P(A)\,P(A_2)\cdots P(A_n) \quad \forall A_2\in \mathcal{A}_2,\dots,A_n\in\mathcal{A}_n\}.\]

The handwritten notes show:

  • $\mathcal{L}$ is a λ-system:
    • Contains $\Omega$,
    • Closed under difference,
    • Closed under increasing unions.
  • $\mathcal{A}_1$ is a π-system.

Thus by Dynkin’s π–λ theorem:

\[\sigma(\mathcal{A}_1) \subset \mathcal{L}.\]

That is:
anything generated by the π-system keeps the independence property.

Repeat cyclically for all indices → independence of all σ-algebras.


5. Example from the Notes (page 2)

We have two random variables $X,Y$.

Given:

\[P(X\le x, Y\le y) = P(X\le x)\, P(Y\le y).\]

Do they have to be independent?

Yes.

Explanation:

  • Sets of the form $(-\infty,x]$ form a π-system (though not a σ-algebra).
  • Independence on this π-system implies independence of the σ-algebras they generate, which are $\sigma(X)$ and $\sigma(Y)$.

Thus $X$ and $Y$ are independent.


6. Example (page 2, bottom)

If ${\mathcal{F}_1,\mathcal{F}_2,\mathcal{F}_3}$ are independent σ-algebras:

  • Then
    \(\sigma(\mathcal{F}_1,\mathcal{F}_2) \quad\text{and}\quad \mathcal{F}_3\) are also independent.

Reason:
$\mathcal{F}_1\cap \mathcal{F}_2$ as a π-system satisfies the required closure.
Apply π–λ again.

Application to random variables

If $X_1,X_2,X_3,X_4,X_5$ are independent random variables, then:

  • $X_1+X_2$
  • $e^{X_3} - \sin(X_1+X_3)$

are independent random variables.

Because the σ-algebras they generate depend only on disjoint subsets of the original independent family.


7. Summary (Lecture 16)

  • Derived Gaussian tail bounds using exponential change-of-variable and Markov/Chernoff ideas.
  • Showed optimized Chebyshev-type inequality.
  • Defined independence of σ-algebras and random variables.
  • Proved independence using π–λ Theorem.
  • Applied independence properties to examples of functions of independent RVs.

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