/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 9 Let \(Y_{1}, Y_{2}, \ldots\) be ... [FREE SOLUTION] | 91Ó°ÊÓ

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Let \(Y_{1}, Y_{2}, \ldots\) be independent, identically distributed random variables with moment generating function \(\psi(t)\) and partial sums \(S_{n}\), \(n \geq 1\left(S_{0}=0\right) .\) Set $$ X_{n}=\frac{e^{t S_{n}}}{(\psi(t))^{n}}, \quad n \geq 1 $$(a) Show that \(X_{1}, X_{2}, \ldots\) is a martingale. (b) Find the relevant martingale if the common distribution is the standard normal one.

Short Answer

Expert verified
The sequence \( \{X_n\} \) is a martingale with \( X_n = e^{t S_n - \frac{nt^2}{2}} \) if the common distribution is standard normal.

Step by step solution

01

Understanding the Definition of a Martingale

A sequence \( \{X_n\} \) is a martingale with respect to a filtration \( \{\mathcal{F}_n\} \) if for all \( n \), \( E[|X_n|] \) is finite and \( E[X_{n+1} | \mathcal{F}_n] = X_n \). In our case, \( \mathcal{F}_n \) is the sigma-algebra generated by \( S_1, S_2, \ldots, S_n \).
02

Check Expectation Given Past Information

Since \( X_n = \frac{e^{t S_n}}{(\psi(t))^n} \), we need to evaluate \( E[X_{n+1} | \mathcal{F}_n] \). Notice that \( S_{n+1} = S_n + Y_{n+1} \), so \( X_{n+1} = \frac{e^{t S_n}e^{t Y_{n+1}}}{(\psi(t))^{n+1}} \).
03

Using Independence of Random Variables

Given \( S_n \), \( Y_{n+1} \) is independent with a moment generating function \( \psi(t) \), hence \( E[e^{t Y_{n+1}} | \mathcal{F}_n] = E[e^{t Y_{n+1}}] = \psi(t) \).
04

Compute the Expectation

Now, \( E[X_{n+1} | \mathcal{F}_n] = E\left[ \frac{e^{t S_n}e^{t Y_{n+1}}}{(\psi(t))^{n+1}} \middle| \mathcal{F}_n \right] = \frac{e^{t S_n}}{(\psi(t))^{n+1}} E[e^{t Y_{n+1}}| \mathcal{F}_n] = \frac{e^{t S_n} \psi(t)}{(\psi(t))^{n+1}} = \frac{e^{t S_n}}{(\psi(t))^n} = X_n \).
05

Conclusion for Part (a)

Since \( E[X_{n+1} | \mathcal{F}_n] = X_n \) for all \( n \), \( \{X_n\} \) is indeed a martingale.
06

Evaluate Standard Normal Distribution Case

For a standard normal random variable \( Y_i \sim N(0,1) \), the moment generating function is \( \psi(t) = e^{t^2/2} \).
07

Martingale with Normal Distribution

Substitute \( \psi(t) = e^{t^2/2} \) into \( X_n = \frac{e^{t S_n}}{(\psi(t))^n} \), yielding \( X_n = e^{t S_n - \frac{nt^2}{2}} \).
08

Conclusion for Part (b)

For standard normal random variables, the martingale is \( X_n = e^{t S_n - \frac{nt^2}{2}} \).

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Moment Generating Functions
Moment Generating Functions (MGFs) are powerful tools in probability theory used to describe the distribution of a random variable. An MGF is defined for a random variable \(Y\) as \(\psi(t) = E[e^{tY}]\), where \(t\) is a real number, and \(E\) denotes the expectation. These functions are useful because they can be employed to find moments (mean, variance, etc.) of the distribution through differentiation at zero. Gravity of MGFs also lies in the fact that they uniquely describe the distribution if it exists in a neighborhood of zero.
MGFs make calculations with sums of independent random variables much more manageable as they allow transformation of the sum's distribution into a product of the MGFs of individual variables. This simplification becomes handy in problems involving independent identically distributed (i.i.d.) variables and calculating expectations under certain constraints.
Independent Identically Distributed Random Variables
Independent Identically Distributed Random Variables, often abbreviated as i.i.d., are a collection of random variables that share the same probability distribution and are mutually independent. This means each variable does not influence the other, and they all have the same statistical properties. This assumption simplifies many statistical models and theories, and it's a common setup for theoretical and practical research.
In our context, if \(Y_1, Y_2, \ldots\) are i.i.d. variables with a common MGF \(\psi(t)\), it indicates that they all share the same probability characteristics, making it easier to analyze cumulative processes like sums \(S_n = Y_1 + Y_2 + \ldots + Y_n\). Understanding the behavior of i.i.d. sequences is crucial for dealing with martingales and applying them across sequentially independent scenarios.
Standard Normal Distribution
The Standard Normal Distribution is a continuous probability distribution that plays a pivotal role in statistics. It's a special case of the normal distribution with a mean of zero \((\mu = 0)\) and a variance of one \((\sigma^2 = 1)\).
The probability density function of a standard normal distribution is symmetric about its mean, resulting in a bell-shaped curve and the moment generating function is \(\psi(t) = e^{t^2/2}\). This MGF helps in characterizing processes that involve standard normal assumptions, like in Part (b) of the exercise where substitution of \(\psi(t)\) reveals the form of the martingale.
Using the standard normal distribution simplifies computation, as many results and properties related to this distribution are well-documented and form the foundation of many statistical inference techniques.
Sigma-algebra
Sigma-algebra is a fundamental concept in measure theory and probability, serving as the foundation for formalizing the notion of "information" in probability spaces. A sigma-algebra \(\mathcal{F}\) on a set \(\Omega\) is a collection of subsets of \(\Omega\) that includes the entire set, the empty set, and is closed under complementation and countable unions.
Sigma-algebras underpin the definition of martingales, providing the structure in which conditional expectations like \(E[X_{n+1} | \mathcal{F}_n]\) are defined. In our exercise, the sigma-algebra \(\mathcal{F}_n\) represents the information up to step \(n\), importantly affecting how we compute expected values and make predictions in a stochastic process.
Expectation in Probability
Expectation, or the expected value, is a fundamental concept in probability theory that calculates the average outcome of a random variable if an experiment is repeated a large number of times. It's denoted by \(E[X]\) for a random variable \(X\), representing the long-run average you would expect.
The expectation is crucial in evaluating the properties of random variables, such as checking whether a sequence \(\{X_n\}\) is a martingale by ensuring that \(E[X_{n+1} | \mathcal{F}_n] = X_n\) as seen in our exercise. Expectation allows us to make educated predictions about outcomes in probabilistic models, ensuring rigorous analysis when conditions, such as independence and identical distribution of random variables, are proposed.

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Most popular questions from this chapter

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