Chapter 4: Problem 6
Let \(X\) be \(N\left(\mu, \sigma^{2}\right)\). Show that \(\mathbb{E}[(X-\mu) g(X)]=\sigma^{2} \mathbb{E}\left(g^{\prime}(X)\right)\) when both sides exist.
Short Answer
Expert verified
The expectation fulfills the equation: \(\mathbb{E}[(X-\mu)g(X)] = \sigma^2 \mathbb{E}[g'(X)]\) through integration by parts.
Step by step solution
01
Understand the expectation
The expression \(\mathbb{E}[(X-\mu)g(X)]\) represents the expectation of the product of \((X-\mu)\) and \(g(X)\) under the assumption that \(X\) follows a normal distribution with parameters \(\mu\) and \(\sigma^2\).
02
Use integration by parts
We start by expressing the expectation \(\mathbb{E}[(X-\mu)g(X)]\) as an integral:\[ \mathbb{E}[(X-\mu)g(X)] = \int_{-\infty}^{\infty} (x-\mu)g(x)f_X(x)\,dx, \]where \(f_X(x)\) is the probability density function of \(X\). We use integration by parts, letting \(u = g(x)\) and \(dv = (x-\mu)f_X(x)\,dx\).
03
Identify \(dv\) and \(v\)
Given \(dv = (x-\mu)f_X(x)\,dx\), and since \(f_X(x)\) for a normal distribution can be written as \[ f_X(x) = \frac{1}{\sqrt{2\pi}\sigma} e^{-\frac{(x-\mu)^2}{2\sigma^2}}, \]integration simplifies \[ v = -\sigma^2 f_X(x) \].
04
Identify \(du\)
\(u = g(x)\) so \(du = g'(x)\,dx\).
05
Apply integration by parts
Substitute back into integration by parts formula: \[ \int u\,dv = uv - \int v\,du. \]Thus, \[ \int (x-\mu)g(x)f_X(x)\,dx = \left[ -\sigma^2 g(x) f_X(x) \right]_{-\infty}^{\infty} + \sigma^2 \int g'(x) f_X(x)\,dx. \] The boundary term goes to zero because \(f_X(x)\) goes to zero at ±∞.
06
Conclusion
The integral evaluates to the arbitrary limits, \[ \sigma^2 \int g'(x) f_X(x)\,dx = \sigma^2 \mathbb{E}[g'(X)]. \] Therefore, we conclude: \[ \mathbb{E}[(X-\mu)g(X)] = \sigma^2 \mathbb{E}[g'(X)] \] as required.
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Key Concepts
These are the key concepts you need to understand to accurately answer the question.
Normal Distribution
A normal distribution is one of the most important concepts in statistics and is often called a Gaussian distribution. It is a continuous probability distribution characterized by a symmetric, bell-shaped curve.
- The distribution is defined by two parameters: the mean \(\mu\), which determines its center, and the variance \(\sigma^2\), which determines its spread.
- The probability density function (pdf) of a normal distribution is given by: \[ f_X(x) = \frac{1}{\sqrt{2\pi}\sigma} e^{-\frac{(x-\mu)^2}{2\sigma^2}}. \]
- This distribution is commonly used in statistics because of the central limit theorem, which states that the sum of a large number of independent, identically distributed variables is approximately normally distributed, regardless of the original distribution.
Integration by Parts
Integration by parts is a fundamental calculus technique used to integrate the product of two functions. Like the product rule for differentiation, it provides a way to break down a complex integration problem into simpler parts. The formula for integration by parts is expressed as:
In the provided solution, integration by parts is employed to handle the expectation \(\mathbb{E}[(X-\mu)g(X)]\). By selecting \(u = g(x)\) and \(dv = (x-\mu)f_X(x)\,dx\), the problem becomes manageable, allowing the transformation of a complex integral into one involving the derivative of \(g(x)\). The trick is to eliminate the difficult term by transferring the differentiation from \(x - \mu\) to \(g(x)\).
- \[ \int u \, dv = uv - \int v \, du. \]
In the provided solution, integration by parts is employed to handle the expectation \(\mathbb{E}[(X-\mu)g(X)]\). By selecting \(u = g(x)\) and \(dv = (x-\mu)f_X(x)\,dx\), the problem becomes manageable, allowing the transformation of a complex integral into one involving the derivative of \(g(x)\). The trick is to eliminate the difficult term by transferring the differentiation from \(x - \mu\) to \(g(x)\).
Expectation Integration
Expectation is a fundamental concept in probability that provides the average or mean value of a random variable over repeated trials. When we talk about expectations involving functions of random variables, integration comes into play. For a continuous random variable \(X\) with pdf \(f_X(x)\), the expectation \(\mathbb{E}[h(X)]\) of a function \(h(x)\) is given by:
- \[ \mathbb{E}[h(X)] = \int_{-\infty}^{\infty} h(x) f_X(x) \, dx. \]