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If \(Y_{1}, \ldots, Y_{n} \stackrel{\text { iid }}{\sim} N\left(\mu, c \mu^{2}\right)\), where \(c\) is a known constant, show that the minimal sufficient statistic for \(\mu\) is the same as for the \(N\left(\mu, \sigma^{2}\right)\) distribution. Find the maximum likelihood estimate of \(\mu\) and give its large-sample standard error. Show that the distribution of \(\bar{Y}^{2} / S^{2}\) does not depend on \(\mu\).

Short Answer

Expert verified
The minimal sufficient statistic for \(\mu\) is \(\bar{Y}\). MLE for \(\mu\) is \(\hat{\mu} = \bar{Y}\). The large-sample standard error is \(\sqrt{\frac{c\hat{\mu}^2}{n}}\).

Step by step solution

01

Identify the Likelihood Function

The likelihood function for the sample \(Y_1, \ldots, Y_n\) from \(N(\mu, c\mu^2)\) is given by:\[ L(\mu) = \prod_{i=1}^{n} \frac{1}{\sqrt{2\pi c\mu^{2}}} \exp\left(-\frac{(Y_i - \mu)^2}{2c\mu^{2}}\right) \].
02

Simplify to Find Sufficient Statistic

Since \( -2 \) times the log-likelihood involves terms like \( \sum_{i=1}^n (Y_i - \mu)^2 \), observe that \( \sum (Y_i)^2, \bar{Y}, n \) appear. By the factorization theorem, the sufficient statistic for \( \mu \) is \(T = (\sum Y_i, \sum Y_i^2, n)\) which is minimized to \(\bar{Y}\) when the distribution is \(N(\mu, \sigma^2)\).
03

Maximum Likelihood Estimation of \(\mu\)

The likelihood is the same subject to the variance in terms of \(\mu\), so the MLE estimator for \(\mu\) following transformations is \(\hat{\mu} = \bar{Y}\), as derived by equating the derivative of the logarithm of the likelihood to zero.
04

Large-Sample Standard Error

The variance for population distribution is limited to \( \frac{c\mu^2}{n} \). Thus, the standard error of the sample mean \(\bar{Y}\) is on approximation \(\sqrt{\frac{c\mu^2}{n}}\), indicating the large-sample standard error gets obtained as \(\sqrt{\frac{c\hat{\mu}^2}{n}}\).
05

Verify Independence of Ratio \(\bar{Y}^2/S^2\)

Given \(\bar{Y}\) and \(S^2\) being statistics containing \(\mu\), substituting their expressions obtains terms cancelling out \(\mu\). Examining \(\bar{Y}=\frac{1}{n}\sum Y_i\) and \(S^2=\frac{1}{n-1}\sum (Y_i-\bar{Y})^2\), the expression \(\bar{Y}^2/S^2\) is independent of \(\mu\), as they rely on derived independent distributions of chi-square and normal.

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Key Concepts

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

Maximum Likelihood Estimation
Maximum Likelihood Estimation, or MLE, is a method used to estimate the parameters of a statistical model. The goal is to find the parameter values that make the observed data most probable. For instance, if our data are believed to follow a normal distribution with unknown mean \(8\), we want to find the \(\u00b5\) that maximizes the likelihood of observing the sample data we have.
  • We start by defining a likelihood function, \(L(\mu)\), which describes how likely each observed data point is, given various possible values of \(\u00b5\).
  • In this exercise, the likelihood function for data \((Y_1, \ldots, Y_n)\) from the normal distribution \(N(\u00b5, c\u00b5^2)\) involves the product of terms involving each \(Y_i\).
  • By taking the derivative of the log-likelihood, we solve for \(\u00b5\) by setting its derivative to zero, leading to the Maximum Likelihood Estimate: \(\hat{\mu} = \bar{Y}\).
Sufficient Statistic
A sufficient statistic is a valuable concept in statistical inference. It summarizes the data in a way that provides all the information needed to estimate a parameter.Essentially, if you know the value of the sufficient statistic, you don't gain any new information about the parameter from knowing the actual data itself.
  • In the given problem, the sufficient statistic for \(\mu\) in a normal distribution \(N(\u00b5, \sigma^2)\) is the sample mean \(\bar{Y}\).
  • By applying the factorization theorem, we identify that the data combination \(T = (\sum Y_i, \sum Y_i^2, n)\) serves as a base to form sufficient statistics.
  • It simplifies further to just the sample mean \(\bar{Y}\), which is a concise summary of the sample conceived as a sufficient statistic when minimizing redundancy.
Statistical Distribution
Statistical distributions describe how values are spread or distributed for a random variable. The normal distribution is fundamental in statistics due to its unique properties.When we say a sample \(Y_1, \ldots, Y_n\) is distributed as \(N(\u00b5, c\u00b5^2)\), we are referring to each data point being normally distributed with mean \(\u00b5\) and variance \(c\u00b5^2\).
  • These parameters (8 and variance) characterize the curve's center and spread, respectively.
  • In practice, many large datasets approximate normality due to the Central Limit Theorem, making this distribution essential for practical analysis.
  • Understanding how \(\mu\) and \(c\u00b5^2\) affect the appearance of the distribution helps in predicting the behavior of the sample data.
Large Sample Theory
Large sample theory, often known as asymptotic theory, deals with the behavior of estimators as the sample size grows larger. It is fundamental in understanding the reliability of statistical estimates for large samples.
  • An engaging example of this theory is the approxi mation of the sampling distribution of the estimator, \(\bar{Y}\), which, as per the Central Limit Theorem, is typically normal or nearly so for large \(n\).
  • As in the provided problem, knowing the population variance \(c\u00b5^2/n\), we derive the standard error that describes spread or variation around \(\hat{\mu}\) for large samples. This simplifies to \(\sqrt{c\u00b5^2/n}\).
  • Thus, large sample theory promises that as sample size increases, the estimates (like the MLE) converge to true parameter values, offering confidence in their use with growing data.

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Most popular questions from this chapter

Find maximum likelihood estimates for \(\theta\) based on a random sample of size \(n\) from the densities (i) \(\theta y^{\theta-1}, 00 ;\) (ii) \(\theta^{2} y e^{-\theta y}, y>0, \theta>0 ;\) and (iii) \((\theta+1) y^{-\theta-2}\), \(y>1, \theta>0\)

In some measurements of \(\mu\)-meson decay by L. Janossy and D. Kiss the following observations were recorded from a four channel discriminator: in 844 cases the decay time was less than 1 second; in 467 cases the decay time was between 1 and 2 seconds; in 374 cases the decay time was between 2 and 3 seconds; and in 564 cases the decay time was greater than 3 seconds. Assuming that decay time has density \(\lambda e^{-\lambda t}, t>0, \lambda>0\), find the likelihood for \(\lambda .\) Find the maximum likelihood estimate, \(\widehat{\lambda}\), find its standard error, and give a \(95 \%\) confidence interval for \(\lambda\). Check whether the data are consistent with an exponential distribution by comparing the observed and fitted frequencies.

\(Y_{1}, \ldots, Y_{n}\) are independent normal random variables with unit variances and means \(\mathrm{E}\left(Y_{j}\right)=\beta x_{j}\), where the \(x_{j}\) are known quantities in \((0,1]\) and \(\beta\) is an unknown parameter. Show that \(\ell(\beta) \equiv-\frac{1}{2} \sum\left(y_{j}-x_{j} \beta\right)^{2}\) and find the expected information \(I(\beta)\) for \(\beta\) Suppose that \(n=10\) and that an experiment to estimate \(\beta\) is to be designed by choosing the \(x_{j}\) appropriately. Show that \(I(\beta)\) is maximized when all the \(x_{j}\) equal \(1 .\) Is this design sensible if there is any possibility that \(\mathrm{E}\left(Y_{j}\right)=\alpha+\beta x_{j}\), with \(\alpha\) unknown?

Let \(\psi(\theta)\) be a 1-1 transformation of \(\theta\), and consider a model with log likelihoods \(\ell(\theta)\) and \(\ell^{*}(\psi)\) in the two parametrizations respectively; \(\ell\) has a unique maximum at which the likelihood equation is satisfied. Show that $$ \frac{\partial \ell^{*}(\psi)}{\partial \psi_{r}}=\frac{\partial \theta^{\mathrm{T}}}{\partial \psi_{r}} \frac{\partial \ell(\theta)}{\partial \theta}, \quad \frac{\partial^{2} \ell^{*}(\psi)}{\partial \psi_{r} \partial \psi_{s}}=\frac{\partial \theta^{\mathrm{T}}}{\partial \psi_{r}} \frac{\partial^{2} \ell(\theta)}{\partial \theta \partial \theta^{\mathrm{T}}} \frac{\partial \theta}{\partial \psi_{s}}+\frac{\partial^{2} \theta^{\mathrm{T}}}{\partial \psi_{r} \partial \psi_{s}} \frac{\partial \ell(\theta)}{\partial \theta} $$ and deduce that $$ I^{*}(\psi)=\frac{\partial \theta^{\mathrm{T}}}{\partial \psi} I(\theta) \frac{\partial \theta}{\partial \psi^{\mathrm{T}}} $$ but that a similar equation holds for observed information only when \(\theta=\widehat{\theta}\).

A location-scale model with parameters \(\mu\) and \(\sigma\) has density $$ f(y ; \mu, \sigma)=\frac{1}{\sigma} g\left(\frac{y-\mu}{\sigma}\right), \quad-\infty0 $$ (a) Show that the information in a single observation has form $$ i(\mu, \sigma)=\sigma^{-2}\left(\begin{array}{ll} a & b \\ b & c \end{array}\right) $$ and express \(a, b\), and \(c\) in terms of \(h(\cdot)=\log g(\cdot) .\) Show that \(b=0\) if \(g\) is symmetric about zero, and discuss the implications for the joint distribution of the maximum likelihood estimators \(\widehat{\mu}\) and \(\widehat{\sigma}\) when \(g\) is regular. (b) Find \(a, b\), and \(c\) for the normal density \((2 \pi)^{-1 / 2} e^{-u^{2} / 2}\) and the log-gamma density \(\exp \left(\kappa u-e^{u}\right) / \Gamma(\kappa)\), where \(\kappa>0\) is known.

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