Problem 9.72 (8 points)
Suppose that
\(Y_1,\dotsc,Y_n\) denote a random sample from a Poisson distribution with mean
\(\lambda > 0\). Then the probability mass function is
\[
p(y \mid \lambda) = e^{-\lambda}\frac{\lambda^y}{y!},
\qquad y = 0,1,2,3,\dotsc
\]
-
We find the likelihood function and the derivative of its natural log.
\[\begin{align*}
L(y_1,\dotsc,y_n \mid \lambda)
&=
\prod_{i=1}^{n} p(y_i \mid \lambda) = e^{-n\lambda}\cdot
\lambda^{\sum_{i=1}^{n}y_i} / (y_1 ! \dotsb y_n !) \\
\implies \ln L(y_1,\dotsc,y_n \mid \lambda)
&=
-n \lambda + \left(\sum_{i=1}^{n} y_i\right) \ln \lambda
- \ln\left(y_1 ! \dotsb y_n !\right) \\
\implies \frac{\partial}{\partial \lambda} \ln L(y_1,\dotsc,y_n \mid \lambda)
&= -n + \frac{1}{\lambda}\sum_{i=1}^{n} y_i.
\end{align*}\]
We see that \(\hat{\lambda}\) is a critical point for the log likelihood if and only if \(\hat{\lambda} = \frac{1}{n}\sum_{i=1}^{n} y_i\). The second derivative test confirms this critical point is a maximum. Therefore, the Maximum Likelihood Estimator for \(\lambda\) is \[
\hat{\lambda} = \frac{1}{n}\sum_{i=1}^{n} Y_i = \overline{Y}.
\]
-
The expected value and variance of the MLE are
\[\begin{align*}
E[\hat{\lambda}] &= E[\overline{Y}] = E[Y] = \lambda \\
V[\hat{\lambda}] &= V[\overline{Y}] = \frac{1}{n}V[Y] = \frac{1}{n}\lambda.
\end{align*}\]
-
Since \[
\lim_{n\rightarrow \infty}V[\hat{\lambda}] =
\lim_{n\rightarrow \infty}\frac{\lambda}{n} = 0,
\] Theorem \(9.1\) implies that \(\hat{\lambda}\) is a consistent estimator for \(E[\hat{\lambda}] = \lambda\).
-
Let \(t(\lambda) = e^{-\lambda} = P(Y = 0)\). The invariance property for Maximum Likelihood Estimators implies that the MLE for \(e^{-\lambda}\) is \[
t(\hat{\lambda}) = t(\overline{Y}) = e^{-\overline{Y}}.
\]
Problem 9.74 (6 points)
Let
\(Y_1,\dotsc,Y_n\) denote a random sample from the probability distribution whose density function is
\[
f_Y(y \mid \theta) =
\begin{cases}
\frac{1}{\theta} r y^{r - 1} e^{-y^r/\theta}, & \theta > 0, y > 0 \\
0, & \textrm{elsewhere}
\end{cases},
\] where
\(r\) is a known positive constant.
-
We write the likelihood function \[
L(y_1,\dotsc,y_n \mid \theta) = \prod_{i=1}^{n} f(y_i \mid \theta) =
\left[
\frac{1}{\theta^n} e^{-\sum_{i=1}^n y_i^r / \theta}
\right]\cdot
\left[
r^n \left(\prod_{i=1}^{n} y_i\right)^{r-1}
\right] =
g(u,\theta)\cdot h(y_1,\dots,y_n),
\] where \(u = \sum_{i=1}^{n} y_i^r\), \(g(u,\theta) = \frac{1}{\theta^n} e^{-u/\theta}\) and \(h(y_1,\dotsc,y_n) = r^n \left(\prod_{i=1}^{n} y_i\right)^{r-1}\). The factorization criterion implies that a minimal sufficient statistic for \(\theta\) is \[
U = \sum_{i=1}^n Y_i^r.
\]
-
Let \(\ell(\theta)\) denote the log likelihood function. Then \[
\ell(\theta) = \ln L(y_1,\dotsc,y_n \mid \theta) =
-n \ln \theta - \frac{1}{\theta}\sum_{i=1}^{n} y_i^r
+ \ln\left[r^n \left(\prod_{i=1}^{n} y_i\right)^{r-1}\right].
\] Then \(\ell'(\theta) = -n \theta^{-1} + \theta^{-2} \sum_{i=1}^{n} y_i^r\), and \(\ell'(\hat{\theta}) = 0\) implies that \(\hat{\theta} = \frac{1}{n}\sum_{i=1}^{n} y_i^r\). A calculation shows that \(\ell''(\hat{\theta}) < 0\), so \(\ell(\theta)\) has a maximum at \(\hat{\theta}\). Therefore, the MLE for \(\theta\) is \[
\hat{\theta} = \frac{1}{n}\sum_{i=1}^{n} Y_i^r.
\]
-
Note that \(\hat{\theta} = \frac{1}{n} U\). From part (a), we know that \(U\) is a minimal sufficient statistic for \(\theta\), so if \(\hat{\theta}\) is unbiased then the Rao-Blackwell Theorem implies that \(\hat{\theta}\) is a MVUE.
Let \(w = y^r\), then \(dw = r y^{r-1} dy\) and \[
f_Y(y \mid \theta)\,dy = \frac{1}{\theta} r y^{r - 1} e^{-y^r/\theta}\,dy =
\frac{1}{\theta} e^{-w/\theta}\,dw = f_W(w \mid \theta)\,dw,
\] which shows that the random variable \(W = Y^r\) has an Exponential distribution with mean \(\theta\). Thus \(E[Y^r] = E[W] = \theta\), and therefore \(E[\hat{\theta}] = \frac{1}{n}\sum_{i=1}^{n} E[Y_i^r] = \theta\), which shows that \(\hat{\theta}\) is an unbiased estimator for \(\theta\) and hence a MVUE for \(\theta\).
Problem 9.77 (10 points)
Let
\(Y_1,\dotsc,Y_n\) denote a random sample from a Gamma distribution whose probability density function is given by
\[
f_Y(y \mid \theta) =
\begin{cases}
\frac{1}{\Gamma(\alpha)\theta^{\alpha}} y^{\alpha - 1} e^{-y/\theta},
& y > 0 \\
0, & \textrm{elsewhere}
\end{cases},
\] where
\(\alpha\) is known.
-
We write the likelihood function \[
L(y_1,\dotsc,y_n \mid \theta) = \prod_{i=1}^{n} f_Y(y_i \mid \theta) =
\left[\Gamma(\alpha) \theta^{\alpha}\right]^{-n}\cdot
\left(\prod_{i=1}^{n} y_i\right)^{\alpha - 1}\cdot
\exp\left(-\frac{1}{\theta}\sum_{i=1}^{n}y_i\right).
\] Let \(\ell(\theta)\) denote the log likelihood function. Then \[
\ell(\theta) = \ln L(y_1,\dotsc,y_n \mid \theta) =
-n \alpha \ln \theta - \frac{1}{\theta}\sum_{i=1}^{n} y_i
+ \ln \left[
\left(\Gamma(\alpha)\right)^{-n} \left(\prod_{i=1}^{n} y_i \right)^{\alpha-1}
\right].
\] The derivative of the log likelihood is \(\ell'(\theta) = -n \alpha \theta^{-1} + \theta^{-2}\sum_{i=1}^{n} y_i\), thus \(\ell'(\hat{\theta}) = 0\) implies \(\hat{\theta} = \frac{1}{n \alpha}\sum_{i=1}^{n}y_i\). A calculation shows that \(\ell''(\hat{\theta}) < 0\), which shows that \(\hat{\theta}\) is a maximum. Therefore, the Maximum Likelihood Estimator for \(\theta\) is \[
\hat{\theta} = \frac{1}{n \alpha}\sum_{i=1}^{n} Y_i
= \frac{1}{\alpha} \overline{Y}.
\]
-
\(Y\) is a Gamma distributed random variable, so \(E[Y] = \alpha \theta\) and \(V[Y] = \alpha \theta^2\). Hence
\[\begin{align*}
E[\hat{\theta}] &= \frac{1}{\alpha}E[\overline{Y}]
= \frac{\alpha \theta}{\alpha} = \theta. \\
V[\hat{\theta}] &= \frac{1}{\alpha^2}V[\overline{Y}]
= \frac{\alpha \theta^2}{n\alpha^2} = \frac{\theta^2}{n\alpha}.
\end{align*}\]
-
Since \[
\lim_{n\rightarrow \infty}V[\hat{\theta}]
= \lim_{n\rightarrow \infty} \frac{\theta^2}{n\alpha} = 0,
\] Theorem \(9.1\) shows that \(\hat{\theta}\) is a consistent estimator for \(E[\hat{\theta}] = \theta\).
-
We rewrite the likelihood function as
\[\begin{align*}
L(y_1,\dotsc,y_n \mid \theta) &=
\left[
\theta^{-n\alpha}e^{-\frac{1}{\theta}\sum_{i=1}^{n} y_i}
\right]\cdot
\left[
\left(\Gamma(\alpha)\right)^{-n}
\left(\prod_{i=1}^{n}y_i\right)^{\alpha - 1}
\right] \\
&= g(u,\theta)\cdot h(y_1,\dotsc,y_n),
\end{align*}\]
where \(u = \sum_{i=1}^{n} y_i\). By the factorization criterion, \[
U = \sum_{i=1}^{n} Y_i
\] is a minimal sufficient statistic for \(\theta\).
-
Let \(n = 5\) and \(\alpha = 2\). Since \(Y\) has a Gamma distribution with \(\alpha = 2\) and \(\beta = \theta\), Problem \(6.40\) shows that \(W = \frac{2}{\theta} Y\) has a \(\chi^2\)-distribution with \(\nu = 2\alpha = 4\) degrees of freedom. Thus \[
\frac{2}{\theta}U = \frac{2}{\theta}\sum_{i=1}^{5} Y_i
\] has a \(\chi^2\)-distribution with \(\nu=20\) degrees of freedom. Using this as a pivotal quantity we find
\[\begin{align*}
P\left(\chi^{2}_{0.95} \le \frac{2}{\theta}U \le \chi^{2}_{0.05}\right)
&= 0.90 \\
P\left(\frac{2U}{\chi^{2}_{0.05}} \le \theta \le \frac{2U}{\chi^{2}_{0.95}}\right)
&= 0.90.
\end{align*}\]
With \(\nu = 20\), \(\chi^{2}_{0.05} = 31.4104\), \(\chi^{2}_{0.95} = 10.8508\). Therefore, a \(90\%\) confidence interval for \(\theta\) is \[
\left(0.0637\sum_{i=1}^{5} Y_i , 0.1843\sum_{i=1}^{5} Y_i\right)
\]
Problem 9.80 (2 points)
Let
\(Y_1,\dotsc,Y_n\) denote a random sample from a probability distribution whose density function is given by
\[
f_Y(y \mid \theta) =
\begin{cases}
(\theta + 1) y^{\theta}, & 0 < y < 1, \theta > -1 \\
0, & \textrm{elsewhere}
\end{cases}.
\] We write the likelihood function
\[
L(y_1,\dotsc,y_n \mid \theta) = \prod_{i=1}^{n} f_Y(y_i \mid \theta)
= (\theta + 1)^{n} \left(\prod_{i=1}^{n} y_i\right)^{\theta}.
\] Let
\(\ell(\theta)\) denote the log likelihood function. Then
\[\begin{align*}
\ell(\theta) &= \ln L(y_1,\dotsc,y_n \mid \theta)
= n \ln (\theta + 1)
+ \theta \ln\left(\prod_{i=1}^{n} y_i\right) \\
\implies
\ell'(\theta) &= \frac{n}{\theta + 1} + \ln\left(\prod_{i=1}^{n} y_i\right).
\end{align*}\]
A calculation shows that \(\ell'(\hat{\theta}) = 0\) if \[
\hat{\theta} =
-\frac{n + \ln \prod_{i=1}^{n} y_i}
{\ln \prod_{i=1}^{n} y_i}.
\] Therefore, the Maximum Likelihood Estimator for \(\theta\) is \[
\hat{\theta} =
-\frac{n + \ln \prod_{i=1}^{n} Y_i}
{\ln \prod_{i=1}^{n} Y_i},
\] which is quite different from the Method Of Moments estimator \((2\overline{Y} - 1)/(1 - \overline{Y})\).
Problem 9.82 (2 points)
\[\begin{align*}
L(p) &= \left[p^{25}(1-p)^{75}\right]\cdot
\left[p^{30}(1-p)^{70}\right]
= p^{55}(1-p)^{145} \\
\ell(p) &= \ln L(p) = 30 \ln p + 145 \ln (1 - p) \\
\ell'(p) &= \frac{30}{p} - \frac{145}{1-p} =
\frac{55(1 - p) - 145p}{p(1 - p)} \\
\ell'(p) &= \frac{55 - 200 p}{p(1 - p)}.
\end{align*}\]
We see that \(\ell'(\hat{p}) = 0\) if and only if \(\hat{p} = 55/200 = 0.275\). Since \(\ell''(\hat{p}) < 0\), we see that the MLE is \(\hat{p} = 0.275\).
Problem 9.84 (6 points)
Let
\(Y_1,\dotsc,Y_n\) be a random sample from a population whose density function is
\[
f(y \mid \theta) =
\begin{cases}
\frac{3y^2}{\theta^3}, & 0 \le y \le \theta \\
0, & \textrm{elsewhere}
\end{cases}.
\] Exercise
\(9.44\) showed that
\(Y_{(n)} = \max(Y_1,\dotsc,Y_n)\) is sufficient for
\(\theta\).
-
We write the likelihood function \[
L(y_1,\dotsc,y_n \mid \theta) = \prod_{i=1}^{n} f(y_i \mid \theta)
= 3^{n}\left(\prod_{i=1}^{n} y_i\right)^{2}
\theta^{-3n}\prod_{i=1}^{n} I_{[0,\theta]}(y_i).
\] As a function of \(\theta\), \(\prod_{i=1}^{n} I_{[0,\theta]}(y_i) = I_{[0,\theta]}(y_{(n)})\cdot I_{[0,\infty)}(y_{(1)}) = 1\) for \(\theta \ge y_{(n)}\), and equals \(0\) for \(\theta < y_{(n)}\). Since \(\theta^{-3n}\) is a decreasing function of \(\theta\), we conclude that \(L(y_1,\dotsc,y_n \mid \theta)\) achieves its maximum value at \(\hat{\theta} = y_{(n)}\). Therefore \(Y_{(n)}\) is a Maximum Likelihood Estimator for \(\theta\).
-
The Cumulative Distribution Function (CDF) for \(Y\) is \[
F_Y(y) = P(Y \le y) =
\begin{cases}
1, & y > \theta \\
(y / \theta)^{3}, & 0 \le y \le \theta \\
0, & y < 0
\end{cases}.
\] From this we deduce that the CDF for \(Y_{(n)}\) is \(G_{(n)}(y) = P(Y_{(n)} \le y) = [F_Y(y)]^{n}\). The corresponding Probability Density Function (PDF) for \(Y_{(n)}\) is \(g_{(n)}(y) = G'_{(n)}(y)\), \[
g_{(n)}(y) =
\begin{cases}
\frac{3n}{\theta^{3n}} y^{3n - 1}, & 0 \le y \le \theta \\
0, & \textrm{elsewhere}
\end{cases}.
\] A quick calculation shows that if we let \(w = y/\theta\), then \(g_{(n)}(y)\) transforms into the density function \[
f_W(w) =
\begin{cases}
3n w^{3n - 1}, & 0 \le w \le 1 \\
0, & \textrm{elsewhere}
\end{cases},
\] which shows that \(W = \frac{1}{\theta}Y_{(n)}\) has a Beta distribution with parameters \(\alpha = 3n\) and \(\beta = 1\). Moreover, since \(f_W(w)\) is independent of \(\theta\), \(W\) is a pivotal quantity.
-
Another quick calculation shows that the CDF for \(W\) is \[
F_W(w) =
\begin{cases}
1, & w > 1 \\
w^{3n}, & 0 \le w \le 1 \\
0, & w < 0
\end{cases}.
\] Let \(0 < \alpha < 1\), then
\[\begin{align*}
P\left((\alpha/2)^{\frac{1}{3n}} \le W
\le (1 - \alpha/2)^{\frac{1}{3n}}\right)
&=
F_W\left((1 - \alpha/2)^{\frac{1}{3n}}\right) -
F_W\left((\alpha/2)^{\frac{1}{3n}}\right) \\
&=
1 - \alpha/2 - \alpha/2 \\
&=
1 - \alpha.
\end{align*}\]
Since \(W = Y_{(n)} / \theta\) and since \[
P\left((\alpha/2)^{\frac{1}{3n}} \le Y_{(n)}/\theta
\le (1 - \alpha/2)^{\frac{1}{3n}}\right)
=
P\left( (1 - \alpha/2)^{-\frac{1}{3n}} Y_{(n)} \le \theta
\le (\alpha/2)^{-\frac{1}{3n}} Y_{(n)}\right),
\] we deduce that a \((1 - \alpha)\cdot 100\%\) confidence interval for \(\theta\) is \[
\left( (1 - \alpha/2)^{-\frac{1}{3n}} Y_{(n)} ,
(\alpha/2)^{-\frac{1}{3n}} Y_{(n)}\right).
\]
Problem 9.86 (2 Points)
Let
\(\beta = t(\theta)\) be an invertible function. Let
\(\hat{\theta}\) be a maximum likelihood estimator for the likelihood function
\(L(y_1,\dotsc,y_n \mid \theta)\), then
\[\begin{equation}
L(y_1,\dotsc,y_n \mid \theta) \le L(y_1,\dotsc,y_n \mid \hat{\theta})
\end{equation}\]
for all \(\theta\).
Let
\(\mathscr{L}(y_1,\dotsc,y_n \mid \beta)\) be the corresponding likelihood function involving
\(\beta\). The two likelihood functions are related as follows:
\[\begin{equation}
L(y_1,\dotsc,y_n \mid \theta) = \mathscr{L}(y_1,\dotsc,y_n \mid t(\theta)).
\end{equation}\]
For example, let
\(Y\) be a normal random variable with
\(E[Y] = 0\) and
\(V[Y] = \sigma^2\),
\(\sigma > 0\). Let
\(t(x) = x^2\), let
\(\theta = \sigma\), then
\(\beta = t(\theta) = \theta^2 = \sigma^2\), and
\[\begin{align*}
\mathscr{L}(y_1,\dotsc,y_n \mid \beta)
&=
\prod_{i=1}^{n} \left(2 \pi \beta \right)^{-1/2} e^{-\frac{1}{2}y_i^2 / \beta}. \\
L(y_1,\dotsc,y_n \mid \theta)
&=
\prod_{i=1}^{n} \left(2 \pi \theta^2 \right)^{-1/2} e^{-\frac{1}{2}y_i^2 / \theta^2} \\
&=
\mathscr{L}(y_1,\dotsc,y_n \mid \theta^2) \\
&=
\mathscr{L}(y_1,\dotsc,y_n \mid t(\theta)).
\end{align*}\]
Returning to the general case, let \(\beta\) be arbitrary, then since \(t\) is invertible we define \(\theta = t^{-1}(\beta)\). Thus, \[
\mathscr{L}(y_1,\dotsc,y_n \mid \beta) =
L(y_1,\dotsc,y_n \mid \theta) \le
L(y_1,\dotsc,y_n \mid \hat{\theta}) =
\mathscr{L}(y_1,\dotsc,y_n \mid t(\hat{\theta})).
\] Since \(\mathscr{L}(y_1,\dotsc,y_n \mid \beta) \le \mathscr{L}(y_1,\dotsc,y_n \mid t(\hat{\theta}))\) for all \(\beta\), \(t(\hat{\theta})\) is a Maximum Likelihood Estimator for \(\beta\).
Problem 9.88 (2 points)
Let \(Y_1,\dotsc,Y_n\) be a random sample from a normal distribution with mean \(\mu\) and variance \(\sigma^2\), both unknown. Example \(9.15\) (pages \(450 - 451\)) shows that \[
\hat{\mu} = \overline{Y},\qquad
\widehat{\sigma^2} =
\frac{1}{n}\sum_{i=1}^{n}\left(Y_i - \overline{Y}\right)^2
\] are Maximum Likelihood Estimators for \(\mu\) and \(\sigma^2\). Since \(\sigma = \sqrt{\sigma^2}\), the invariance property for MLEs implies that \[
\hat{\sigma} = \sqrt{
\frac{1}{n}\sum_{i=1}^{n}\left(Y_i - \overline{Y}\right)^2
}
\] is an MLE for \(\sigma\).
---
title: "Solutions to Homework Assignment 10"
output: html_notebook
---

##Problem 9.72 (8 points)
Suppose that \(Y_1,\dotsc,Y_n\) denote a random sample from
a Poisson distribution with mean \(\lambda > 0\). Then the 
probability mass function is
\[
p(y \mid \lambda) = e^{-\lambda}\frac{\lambda^y}{y!},
\qquad y = 0,1,2,3,\dotsc
\]
<ol type="a">
<li>We find the likelihood function and the derivative of its natural log.
\begin{align*}
L(y_1,\dotsc,y_n \mid \lambda)
&=
\prod_{i=1}^{n} p(y_i \mid \lambda) = e^{-n\lambda}\cdot 
\lambda^{\sum_{i=1}^{n}y_i} / (y_1 ! \dotsb y_n !) \\
\implies \ln L(y_1,\dotsc,y_n \mid \lambda)
&=
-n \lambda + \left(\sum_{i=1}^{n} y_i\right) \ln \lambda
- \ln\left(y_1 ! \dotsb y_n !\right) \\
\implies \frac{\partial}{\partial \lambda} \ln L(y_1,\dotsc,y_n \mid \lambda)
&= -n + \frac{1}{\lambda}\sum_{i=1}^{n} y_i.
\end{align*}
We see that \(\hat{\lambda}\) is a critical point for the log likelihood if and
only if \(\hat{\lambda} = \frac{1}{n}\sum_{i=1}^{n} y_i\). The second
derivative test confirms this critical point is a maximum. Therefore, the
Maximum Likelihood Estimator for \(\lambda\) is
\[
\hat{\lambda} = \frac{1}{n}\sum_{i=1}^{n} Y_i = \overline{Y}.
\]
</li>
<li>
The expected value and variance of the MLE are
\begin{align*}
E[\hat{\lambda}] &= E[\overline{Y}] = E[Y] = \lambda \\
V[\hat{\lambda}] &= V[\overline{Y}] = \frac{1}{n}V[Y] = \frac{1}{n}\lambda.
\end{align*}
</li>
<li>
Since
\[
\lim_{n\rightarrow \infty}V[\hat{\lambda}] =
\lim_{n\rightarrow \infty}\frac{\lambda}{n} = 0,
\]
Theorem \(9.1\) implies that \(\hat{\lambda}\) is a consistent estimator for
\(E[\hat{\lambda}] = \lambda\).
</li>
<li>
Let \(t(\lambda) = e^{-\lambda} = P(Y = 0)\). The invariance property for Maximum
Likelihood Estimators implies that the MLE for \(e^{-\lambda}\) is
\[
t(\hat{\lambda}) = t(\overline{Y}) = e^{-\overline{Y}}.
\]
</li>
</ol>

##Problem 9.74 (6 points)
Let \(Y_1,\dotsc,Y_n\) denote a random sample from the probability distribution
whose density function is
\[
f_Y(y \mid \theta) =
\begin{cases}
\frac{1}{\theta} r y^{r - 1} e^{-y^r/\theta}, & \theta > 0, y > 0 \\
0, & \textrm{elsewhere}
\end{cases},
\]
where \(r\) is a known positive constant.
<ol type="a">
<li>
We write the likelihood function
\[
L(y_1,\dotsc,y_n \mid \theta) = \prod_{i=1}^{n} f(y_i \mid \theta) =
\left[
\frac{1}{\theta^n} e^{-\sum_{i=1}^n y_i^r / \theta}
\right]\cdot
\left[
r^n \left(\prod_{i=1}^{n} y_i\right)^{r-1}
\right] =
g(u,\theta)\cdot h(y_1,\dots,y_n),
\]
where \(u = \sum_{i=1}^{n} y_i^r\), \(g(u,\theta) = \frac{1}{\theta^n} e^{-u/\theta}\) 
and \(h(y_1,\dotsc,y_n) = r^n \left(\prod_{i=1}^{n} y_i\right)^{r-1}\).
The factorization criterion implies that a minimal sufficient statistic for
\(\theta\) is
\[
U = \sum_{i=1}^n Y_i^r.
\]
</li>
<li>
Let \(\ell(\theta)\) denote the log likelihood function. Then
\[
\ell(\theta) = \ln L(y_1,\dotsc,y_n \mid \theta) =
-n \ln \theta - \frac{1}{\theta}\sum_{i=1}^{n} y_i^r 
+ \ln\left[r^n \left(\prod_{i=1}^{n} y_i\right)^{r-1}\right].
\]
Then \(\ell'(\theta) = -n \theta^{-1} + \theta^{-2} \sum_{i=1}^{n} y_i^r\),
and \(\ell'(\hat{\theta}) = 0\) implies that 
\(\hat{\theta} = \frac{1}{n}\sum_{i=1}^{n} y_i^r\). A calculation shows
that \(\ell''(\hat{\theta}) < 0\), so \(\ell(\theta)\) has a maximum at 
\(\hat{\theta}\). Therefore, the MLE for \(\theta\) is
\[
\hat{\theta} = \frac{1}{n}\sum_{i=1}^{n} Y_i^r.
\]
</li>
<li>
Note that \(\hat{\theta} = \frac{1}{n} U\). From part (a), we know that
\(U\) is a minimal sufficient statistic for \(\theta\), so if
\(\hat{\theta}\) is unbiased then the Rao-Blackwell Theorem implies that
\(\hat{\theta}\) is a MVUE.

Let \(w = y^r\), then \(dw = r y^{r-1} dy\) and
\[
f_Y(y \mid \theta)\,dy = \frac{1}{\theta} r y^{r - 1} e^{-y^r/\theta}\,dy =
\frac{1}{\theta} e^{-w/\theta}\,dw = f_W(w \mid \theta)\,dw,
\]
which shows that the random variable \(W = Y^r\) has an Exponential distribution
with mean \(\theta\). Thus \(E[Y^r] = E[W] = \theta\), and therefore
\(E[\hat{\theta}] = \frac{1}{n}\sum_{i=1}^{n} E[Y_i^r] = \theta\), which shows
that \(\hat{\theta}\) is an unbiased estimator for \(\theta\) and hence a 
MVUE for \(\theta\).
</li>
</ol>

##Problem 9.77 (10 points)
Let \(Y_1,\dotsc,Y_n\) denote a random sample from a Gamma distribution whose
probability density function is given by
\[
f_Y(y \mid \theta) =
\begin{cases}
\frac{1}{\Gamma(\alpha)\theta^{\alpha}} y^{\alpha - 1} e^{-y/\theta},
& y > 0 \\
0, & \textrm{elsewhere}
\end{cases},
\]
where \(\alpha\) is known.
<ol type="a">
<li>
We write the likelihood function
\[
L(y_1,\dotsc,y_n \mid \theta) = \prod_{i=1}^{n} f_Y(y_i \mid \theta) =
\left[\Gamma(\alpha) \theta^{\alpha}\right]^{-n}\cdot
\left(\prod_{i=1}^{n} y_i\right)^{\alpha - 1}\cdot
\exp\left(-\frac{1}{\theta}\sum_{i=1}^{n}y_i\right).
\]
Let \(\ell(\theta)\) denote the log likelihood function. Then
\[
\ell(\theta) = \ln L(y_1,\dotsc,y_n \mid \theta) =
-n \alpha \ln \theta - \frac{1}{\theta}\sum_{i=1}^{n} y_i 
+ \ln \left[
\left(\Gamma(\alpha)\right)^{-n} \left(\prod_{i=1}^{n} y_i \right)^{\alpha-1}
\right].
\]
The derivative of the log likelihood is
\(\ell'(\theta) = -n \alpha \theta^{-1} +
\theta^{-2}\sum_{i=1}^{n} y_i\), thus \(\ell'(\hat{\theta}) = 0\) implies
\(\hat{\theta} = \frac{1}{n \alpha}\sum_{i=1}^{n}y_i\). A calculation shows that
\(\ell''(\hat{\theta}) < 0\), which shows that \(\hat{\theta}\) is a maximum.
Therefore, the Maximum Likelihood Estimator for \(\theta\) is
\[
\hat{\theta} = \frac{1}{n \alpha}\sum_{i=1}^{n} Y_i 
= \frac{1}{\alpha} \overline{Y}.
\]
</li>
<li>
\(Y\) is a Gamma distributed random variable, so \(E[Y] = \alpha \theta\)
and \(V[Y] = \alpha \theta^2\). Hence
\begin{align*}
E[\hat{\theta}] &= \frac{1}{\alpha}E[\overline{Y}] 
= \frac{\alpha \theta}{\alpha} = \theta. \\
V[\hat{\theta}] &= \frac{1}{\alpha^2}V[\overline{Y}]
= \frac{\alpha \theta^2}{n\alpha^2} = \frac{\theta^2}{n\alpha}.
\end{align*}
</li>
<li>
Since
\[
\lim_{n\rightarrow \infty}V[\hat{\theta}] 
= \lim_{n\rightarrow \infty} \frac{\theta^2}{n\alpha} = 0,
\]
Theorem \(9.1\) shows that \(\hat{\theta}\) is a consistent estimator 
for \(E[\hat{\theta}] = \theta\).
</li>
<li>
We rewrite the likelihood function as
\begin{align*}
L(y_1,\dotsc,y_n \mid \theta) &=
\left[
\theta^{-n\alpha}e^{-\frac{1}{\theta}\sum_{i=1}^{n} y_i}
\right]\cdot
\left[
\left(\Gamma(\alpha)\right)^{-n}
\left(\prod_{i=1}^{n}y_i\right)^{\alpha - 1}
\right] \\
&= g(u,\theta)\cdot h(y_1,\dotsc,y_n),
\end{align*}
where \(u = \sum_{i=1}^{n} y_i\). By the factorization criterion,
\[
U = \sum_{i=1}^{n} Y_i
\]
is a minimal sufficient statistic for \(\theta\).
</li>
<li>
Let \(n = 5\) and \(\alpha = 2\). Since \(Y\) has a Gamma distribution with
\(\alpha = 2\) and \(\beta = \theta\), Problem \(6.40\) shows that 
\(W = \frac{2}{\theta} Y\) has a
\(\chi^2\)-distribution with \(\nu = 2\alpha = 4\) degrees of freedom.
Thus 
\[
\frac{2}{\theta}U = \frac{2}{\theta}\sum_{i=1}^{5} Y_i
\]
has a \(\chi^2\)-distribution with \(\nu=20\) degrees of freedom.
Using this as a pivotal quantity we find
\begin{align*}
P\left(\chi^{2}_{0.95} \le \frac{2}{\theta}U \le \chi^{2}_{0.05}\right)
&= 0.90 \\
P\left(\frac{2U}{\chi^{2}_{0.05}} \le \theta \le \frac{2U}{\chi^{2}_{0.95}}\right)
&= 0.90.
\end{align*}
With \(\nu = 20\), \(\chi^{2}_{0.05} = 31.4104\), \(\chi^{2}_{0.95} = 10.8508\).
Therefore, a \(90\%\) confidence interval for \(\theta\) is
\[
\left(0.0637\sum_{i=1}^{5} Y_i , 0.1843\sum_{i=1}^{5} Y_i\right)
\]
</li>
</ol>

##Problem 9.80 (2 points)
Let \(Y_1,\dotsc,Y_n\) denote a random sample from a probability distribution
whose density function is given by
\[
f_Y(y \mid \theta) =
\begin{cases}
(\theta + 1) y^{\theta}, & 0 < y < 1, \theta > -1 \\
0, & \textrm{elsewhere}
\end{cases}.
\]
We write the likelihood function
\[
L(y_1,\dotsc,y_n \mid \theta) = \prod_{i=1}^{n} f_Y(y_i \mid \theta) 
= (\theta + 1)^{n} \left(\prod_{i=1}^{n} y_i\right)^{\theta}.
\]
Let \(\ell(\theta)\) denote the log likelihood function. Then
\begin{align*}
\ell(\theta) &= \ln L(y_1,\dotsc,y_n \mid \theta)
= n \ln (\theta + 1) 
+ \theta \ln\left(\prod_{i=1}^{n} y_i\right) \\
\implies
\ell'(\theta) &= \frac{n}{\theta + 1} + \ln\left(\prod_{i=1}^{n} y_i\right).
\end{align*}
A calculation shows that \(\ell'(\hat{\theta}) = 0\) if 
\[
\hat{\theta} = 
-\frac{n + \ln \prod_{i=1}^{n} y_i}
{\ln \prod_{i=1}^{n} y_i}.
\]
Therefore, the Maximum Likelihood Estimator for \(\theta\) is
\[
\hat{\theta} = 
-\frac{n + \ln \prod_{i=1}^{n} Y_i}
{\ln \prod_{i=1}^{n} Y_i},
\]
which is quite different from the Method Of Moments estimator \((2\overline{Y} - 1)/(1 - \overline{Y})\).

##Problem 9.82 (2 points)
\begin{align*}
L(p) &= \left[p^{25}(1-p)^{75}\right]\cdot
\left[p^{30}(1-p)^{70}\right] 
= p^{55}(1-p)^{145} \\
\ell(p) &= \ln L(p) = 30 \ln p + 145 \ln (1 - p) \\
\ell'(p) &= \frac{30}{p} - \frac{145}{1-p} =
\frac{55(1 - p) - 145p}{p(1 - p)} \\
\ell'(p) &= \frac{55 - 200 p}{p(1 - p)}.
\end{align*}
We see that \(\ell'(\hat{p}) = 0\) if and only if
\(\hat{p} = 55/200 = 0.275\). Since \(\ell''(\hat{p}) < 0\), we see that the MLE is \(\hat{p} = 0.275\).

##Problem 9.84 (6 points)
Let \(Y_1,\dotsc,Y_n\) be a random sample from a
population whose density function is
\[
f(y \mid \theta) =
\begin{cases}
\frac{3y^2}{\theta^3}, & 0 \le y \le \theta \\
0, & \textrm{elsewhere}
\end{cases}.
\]
Exercise \(9.44\) showed that 
\(Y_{(n)} = \max(Y_1,\dotsc,Y_n)\) is sufficient for
\(\theta\).
<ol type="a">
<li>
We write the likelihood function
\[
L(y_1,\dotsc,y_n \mid \theta) = \prod_{i=1}^{n} f(y_i \mid \theta)
= 3^{n}\left(\prod_{i=1}^{n} y_i\right)^{2}
\theta^{-3n}\prod_{i=1}^{n} I_{[0,\theta]}(y_i).
\]
As a function of \(\theta\), \(\prod_{i=1}^{n} I_{[0,\theta]}(y_i) = I_{[0,\theta]}(y_{(n)})\cdot I_{[0,\infty)}(y_{(1)}) = 1\) for \(\theta \ge y_{(n)}\), and equals \(0\) for \(\theta < y_{(n)}\). Since
\(\theta^{-3n}\) is a decreasing function of \(\theta\), we conclude that 
\(L(y_1,\dotsc,y_n \mid \theta)\) achieves its maximum 
value at \(\hat{\theta} = y_{(n)}\). Therefore
\(Y_{(n)}\) is a Maximum Likelihood Estimator for 
\(\theta\).
</li>
<li>
The Cumulative Distribution Function (CDF) for \(Y\) is
\[
F_Y(y) = P(Y \le y) = 
\begin{cases}
1, & y > \theta \\
(y / \theta)^{3}, & 0 \le y \le \theta \\
0, & y < 0
\end{cases}.
\]
From this we deduce that the CDF for \(Y_{(n)}\) is \(G_{(n)}(y) = P(Y_{(n)} \le y) = [F_Y(y)]^{n}\).
The corresponding Probability Density Function (PDF)
for \(Y_{(n)}\) is \(g_{(n)}(y) = G'_{(n)}(y)\),
\[
g_{(n)}(y) =
\begin{cases}
\frac{3n}{\theta^{3n}} y^{3n - 1}, & 0 \le y \le \theta \\
0, & \textrm{elsewhere}
\end{cases}.
\]
A quick calculation shows that if we let \(w =  y/\theta\),
then \(g_{(n)}(y)\) transforms into the density function
\[
f_W(w) = 
\begin{cases}
3n w^{3n - 1}, & 0 \le w \le 1 \\
0, & \textrm{elsewhere}
\end{cases},
\]
which shows that \(W = \frac{1}{\theta}Y_{(n)}\) has
a Beta distribution with parameters \(\alpha = 3n\)
and \(\beta = 1\). Moreover, since \(f_W(w)\) is 
independent of \(\theta\), \(W\) is a pivotal
quantity.
</li>
<li>
Another quick calculation shows that the CDF for \(W\)
is
\[
F_W(w) =
\begin{cases}
1, & w > 1 \\
w^{3n}, & 0 \le w \le 1 \\
0, & w < 0
\end{cases}.
\]
Let \(0 < \alpha < 1\), then
\begin{align*}
P\left((\alpha/2)^{\frac{1}{3n}} \le W 
\le (1 - \alpha/2)^{\frac{1}{3n}}\right) 
&=
F_W\left((1 - \alpha/2)^{\frac{1}{3n}}\right) -
F_W\left((\alpha/2)^{\frac{1}{3n}}\right) \\
&=
1 - \alpha/2 - \alpha/2 \\
&= 
1 - \alpha.
\end{align*}
Since \(W = Y_{(n)} / \theta\) and since
\[
P\left((\alpha/2)^{\frac{1}{3n}} \le Y_{(n)}/\theta 
\le (1 - \alpha/2)^{\frac{1}{3n}}\right)
=
P\left( (1 - \alpha/2)^{-\frac{1}{3n}} Y_{(n)} \le \theta 
\le (\alpha/2)^{-\frac{1}{3n}} Y_{(n)}\right),
\]
we deduce that a \((1 - \alpha)\cdot 100\%\) confidence
interval for \(\theta\) is
\[
\left( (1 - \alpha/2)^{-\frac{1}{3n}} Y_{(n)} ,
(\alpha/2)^{-\frac{1}{3n}} Y_{(n)}\right).
\]
</li>
</ol>

##Problem 9.86 (2 Points)
Let \(\beta = t(\theta)\) be an invertible
function. Let \(\hat{\theta}\) be a
maximum likelihood estimator for the
likelihood function
\(L(y_1,\dotsc,y_n \mid \theta)\), then
\begin{equation}
L(y_1,\dotsc,y_n \mid \theta) \le L(y_1,\dotsc,y_n \mid \hat{\theta})
\end{equation}
for all \(\theta\).

Let \(\mathscr{L}(y_1,\dotsc,y_n \mid \beta)\) be the corresponding likelihood
function involving \(\beta\). The two likelihood functions are related
as follows:
\begin{equation}
L(y_1,\dotsc,y_n \mid \theta) = \mathscr{L}(y_1,\dotsc,y_n \mid t(\theta)).
\end{equation}

For example, let \(Y\) be a normal random variable with
\(E[Y] = 0\) and \(V[Y] = \sigma^2\), \(\sigma > 0\). 
Let \(t(x) = x^2\), let \(\theta = \sigma\), then 
\(\beta = t(\theta) = \theta^2 = \sigma^2\), and
\begin{align*}
\mathscr{L}(y_1,\dotsc,y_n \mid \beta)
&=
\prod_{i=1}^{n} \left(2 \pi \beta \right)^{-1/2} e^{-\frac{1}{2}y_i^2 / \beta}. \\
L(y_1,\dotsc,y_n \mid \theta)
&=
\prod_{i=1}^{n} \left(2 \pi \theta^2 \right)^{-1/2} e^{-\frac{1}{2}y_i^2 / \theta^2} \\
&=
\mathscr{L}(y_1,\dotsc,y_n \mid \theta^2) \\
&=
\mathscr{L}(y_1,\dotsc,y_n \mid t(\theta)).
\end{align*}

Returning to the general case, let \(\beta\) be arbitrary, then
since \(t\) is invertible we define \(\theta = t^{-1}(\beta)\).
Thus,
\[
\mathscr{L}(y_1,\dotsc,y_n \mid \beta) =
L(y_1,\dotsc,y_n \mid \theta) \le
L(y_1,\dotsc,y_n \mid \hat{\theta}) =
\mathscr{L}(y_1,\dotsc,y_n \mid t(\hat{\theta})).
\]
Since 
\(\mathscr{L}(y_1,\dotsc,y_n \mid \beta) \le 
\mathscr{L}(y_1,\dotsc,y_n \mid t(\hat{\theta}))\)
for all \(\beta\), \(t(\hat{\theta})\) is a Maximum
Likelihood Estimator for \(\beta\).

##Problem 9.88 (2 points)
Let \(Y_1,\dotsc,Y_n\) be a random sample from a normal distribution
with mean \(\mu\) and variance \(\sigma^2\), both unknown.
Example \(9.15\) (pages \(450 - 451\)) shows that
\[
\hat{\mu} = \overline{Y},\qquad
\widehat{\sigma^2} =
\frac{1}{n}\sum_{i=1}^{n}\left(Y_i - \overline{Y}\right)^2
\]
are Maximum Likelihood Estimators for \(\mu\) and \(\sigma^2\).
Since \(\sigma = \sqrt{\sigma^2}\), the invariance property for
MLEs implies that
\[
\hat{\sigma} = \sqrt{
\frac{1}{n}\sum_{i=1}^{n}\left(Y_i - \overline{Y}\right)^2
}
\]
is an MLE for \(\sigma\).













