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Lecture notes. Written from the material of Berkeley Stat 210A, licensed CC BY 4.0. These are notes, not a transcript: the material has been reorganised and rewritten. This adaptation carries the same licence, and the original is linked above.

77. Sufficiency, Testing, and Bayes: A Final Exam

What this covers

This chapter works through four problems from the Fall 2023 STAT 210A final examination (Prof. Will Fithian), each a self-contained tour through a technique from earlier in the course: exponential-family sufficiency and completeness, maximum likelihood asymptotics and a score test against a non-i.i.d. alternative; hypothesis tests and confidence sets for multivariate normal means alongside a James–Stein-style combined estimator; Rao–Blackwellization, consistency, the delta method, and the continuous mapping theorem in a nonparametric two-sample model; and Bayes point estimation, a minimax lower bound, and a scale-invariant loss function in the uniform scale family. It assumes exponential families and sufficiency/completeness, the Cramér–Rao bound and asymptotic normality of the MLE, the delta method, the James–Stein estimator, and Bayes and minimax risk, all as covered earlier in the course.

1. The Laplace scale family: sufficiency, completeness, and a score test against decay

Let \(X_1, \dots, X_n\) be i.i.d. draws from the Laplace scale family $\(X_i \sim \mathrm{Laplace}(0, \theta) : \quad p_\theta(x) = \frac{1}{2\theta} e^{-|x|/\theta}, \qquad x \in \mathbb{R}, \ \theta > 0.\)$ The density is supported on all of \(\mathbb{R}\) — this is a genuinely different family from the Laplace location family used elsewhere in the course as a running example, where the unknown parameter shifts the density rather than scaling it.

(a) The absolute value is exponential. For \(0 \le a \le b < \infty\), $\(\begin{aligned} \mathbb{P}(|X_i| \in [a,b]) &= \mathbb{P}(X_i \in [-b,-a]) + \mathbb{P}(X_i \in [a,b]) \\ &= \frac{1}{2}\left(\int_{-b}^{-a} \frac{1}{\theta} e^{x/\theta}\,dx + \int_a^b \frac{1}{\theta} e^{-x/\theta}\,dx\right) \\ &= \int_a^b \frac{1}{\theta} e^{-x/\theta}\,dx = \mathbb{P}(Y \in [a,b]), \end{aligned}\)$ where \(Y \sim \mathrm{Exp}(\theta)\): the density folds the negative half-line onto the positive one, and the two halves' contributions just double the tail. So \(|X_i| \sim \mathrm{Exp}(\theta)\).

(b) A complete sufficient statistic. The likelihood is $\(p(x) = \left(\frac{1}{2\theta}\right)^n \exp\left\{-\frac{1}{\theta}\sum_i |x_i|\right\},\)$ an exponential family with sufficient statistic \(T(X) = \sum_i |X_i|\) and natural parameter \(1/\theta\). Because \(1/\theta\) ranges over all of \((0,\infty)\) — an open interval, so the family has full rank — the standard exponential-family fact applies: \(T(X)\) is complete, and a complete sufficient statistic is automatically minimal.

(c) MLE and its asymptotics. With \(T = \sum_i |X_i|\), the log-likelihood is $\(\ell_n(\theta;X) = -n\log(2\theta) - \frac{1}{\theta}T(X), \qquad \dot\ell_n(\theta;X) = -\frac{n}{\theta} + \frac{T(X)}{\theta^2} = \frac{n}{\theta^2}\left(\frac{T(X)}{n} - \theta\right).\)$ The score vanishes at \(\hat\theta = T/n = \frac{1}{n}\sum_i |X_i|\), and since the sign of \(\dot\ell_n\) matches the sign of \(T/n - \theta\), this is the global maximizer. The Fisher information is $\(J_n(\theta) = \mathrm{Var}_\theta\!\left(\frac{T(X)}{\theta^2}\right) = n\theta^{-4}\,\mathrm{Var}_\theta(|X_i|) = n\theta^{-2},\)$ using \(\mathrm{Var}_\theta(|X_i|) = \theta^2\) for the \(\mathrm{Exp}(\theta)\) variable from part (a). Standard MLE theory then gives $\(\sqrt{n}(\hat\theta_n - \theta) \Rightarrow N(0,\theta^2).\)$

(d) Unbiasedness and the Cramér–Rao bound. Since \(\mathbb{E}_\theta|X_i| = \theta\), the average \(T/n\) is unbiased, with variance \(\theta^2/n\) (an average of \(n\) i.i.d. terms each of variance \(\theta^2\)). This is exactly \(1/J_n(\theta) = \theta^2/n\): the MLE attains the Cramér–Rao lower bound here, not just asymptotically but in finite samples.

(e) A score test against a decaying scale. Suppose instead we worry the scale is shrinking geometrically: \(X_i \sim \mathrm{Laplace}(0, \theta_0(1-\delta)^i)\) for \(i=1,\dots,n\), with \(\theta_0\) known for now, and we want to test \(H_0: \delta = 0\) against \(H_1: \delta > 0\). The log-likelihood is $\(\ell_n(\delta;X) = \sum_i \left[-\log(2\theta_0) - i\log(1-\delta) - \frac{|X_i|/\theta_0}{(1-\delta)^i}\right],\)$ with derivative $\(\dot\ell_n(\delta;X) = \sum_i\left[\frac{i}{1-\delta} - \frac{i|X_i|/\theta_0}{(1-\delta)^{i+1}}\right].\)$ At \(\delta = 0\) this is \(\dot\ell_n(0;X) = \sum_{i=1}^n i(1 - |X_i|/\theta_0)\), and since \(|X_i|/\theta_0 \sim \mathrm{Exp}(1)\) has variance \(1\) under the null, the Fisher information there is $\(J_n(0) = \mathrm{Var}_0(\dot\ell_n(0;X)) = \sum_{i=1}^n i^2 \,\mathrm{Var}(|X_i|/\theta_0) = \sum_{i=1}^n i^2.\)$ The normalized score statistic $\(Z = \frac{\sum_{i=1}^n i(1 - |X_i|/\theta_0)}{\left(\sum_{i=1}^n i^2\right)^{-1/2}} \Rightarrow N(0,1)\)$ (the exam takes the asymptotic normality of this non-i.i.d. score statistic as given) is compared to \(z_\alpha\) for a one-sided test, since the alternative is one-sided.

(f) Removing the nuisance parameter (starred). If \(\theta_0\) is also unknown, the score test above cannot be run directly. The move is to condition on a statistic that is sufficient for \(\theta_0\) under the null submodel: here that is \(T(X) = \sum_i|X_i|\) (part (b)). Substituting the plug-in \(\hat\theta_0 = T/n\) into the score statistic gives $\(W = \frac{\sum_{i=1}^n i(1 - |X_i|n/T)}{\left(\sum_{i=1}^n i^2\right)^{-1/2}},\)$ and rejecting for large \(W\) is equivalent, up to an affine transformation, to rejecting for small values of \(\sum_i i|X_i|/T\). Because \(W\) is a function of \(X/T\) only, its distribution under the null does not depend on \(\theta_0\) at all — it can be found by simulation rather than by an asymptotic argument, restoring finite-sample control of the Type I error. Concretely, under the null the vector \(D = (|X_1|,\dots,|X_n|)/T\) is \(\mathrm{Dirichlet}(\mathbf{1}_n)\) and independent of \(T\), so simulating \(D\) (equivalently, simulating \((|X_1|,\dots,|X_n|)\) given \(T=t\) as \(t \cdot D\)) gives the exact conditional null distribution of the test statistic, from which the cutoff is read off numerically. This is the general principle of building a similar test by conditioning on a sufficient statistic for the nuisance parameter under the null.

2. Multivariate normal means: tests, intervals, and a Stein estimator

Now suppose we observe two independent multivariate normal vectors in \(\mathbb{R}^d\), \(d \ge 3\): $\(X^{(i)} \sim N_d(\theta^{(i)}, \sigma^2 I_d), \quad i=1,2, \qquad \theta^{(1)},\theta^{(2)} \in \mathbb{R}^d.\)$

(a) Known variance: a \(\chi^2\) test. Set \(Y = X^{(2)} - X^{(1)} \sim N_d(\theta^{(2)}-\theta^{(1)}, 2\sigma^2 I_d)\). Under \(H_0: \theta^{(1)} = \theta^{(2)}\), $\(\frac{1}{2\sigma^2}\|Y\|^2 \sim \chi^2_d,\)$ so the test rejects when this exceeds the upper-\(\alpha\) quantile of \(\chi^2_d\).

(b) Unknown variance, common shift: a one-sample \(t\)-test. Suppose now \(\sigma^2\) is unknown but every coordinate is shifted by the same amount, \(\theta^{(2)}_j = \theta^{(1)}_j + \delta\). Then \(Y \sim N_d(\delta\mathbf{1}_d, 2\sigma^2 I_d)\), which is exactly the setup of a one-sample \(t\)-test on the \(d\) "observations" \(Y_1,\dots,Y_d\): reject \(H_0:\delta=0\) against \(\delta \ne 0\) when $\(\frac{|\overline{Y}|}{\sqrt{S^2/d}} > t_{d-1}(\alpha/2),\)$ where \(\overline{Y} = \frac{1}{d}\sum_j Y_j \sim N(\delta, 2\sigma^2/d)\) and \(S^2 = \frac{1}{d-1}\sum_j(Y_j-\overline{Y})^2 \sim \frac{2\sigma^2}{d-1}\chi^2_{d-1}\), independently of \(\overline{Y}\).

(c) Inverting the test for a confidence interval. Testing the point null \(\delta=\delta_0\) shifts the problem to \(Y - \delta_0\mathbf{1}_d \sim N_d((\delta-\delta_0)\mathbf{1}_d, 2\sigma^2 I_d)\), and inverting the rejection region of part (b) gives the interval $\(\overline{Y} \pm \sqrt{S^2/d}\cdot t_{d-1}(\alpha/2).\)$

(d) A Stein estimator built from orthogonal contrasts (starred). Drop the shift assumption, fix \(\sigma^2=1\), and suppose only that we believe \(\theta^{(1)} \approx \theta^{(2)}\) without a strong prior on how. The trick is to rotate to two independent orthogonal contrasts: $\(Z = \frac{X^{(2)}-X^{(1)}}{\sqrt{2}} \sim N_d(\mu, I_d), \qquad W = \frac{X^{(1)}+X^{(2)}}{\sqrt 2} \sim N_d(\nu, I_d),\)$ where \(\mu = (\theta^{(2)}-\theta^{(1)})/\sqrt2\) and \(\nu=(\theta^{(1)}+\theta^{(2)})/\sqrt2\). \(Z\) and \(W\) are independent because they are orthogonal linear images of \((X^{(1)},X^{(2)})\). Since we believe \(\theta^{(1)}\approx\theta^{(2)}\), i.e. \(\mu \approx 0\), apply a James–Stein estimator to \(Z\) but the plain MLE to \(W\): $\(\hat\mu = \left(1 - \frac{d-2}{\|Z\|^2}\right)Z, \qquad \hat\nu = W.\)$ Undoing the rotation, \(\theta^{(2)} = (\mu+\nu)/\sqrt2\) and \(\theta^{(1)} = (\nu-\mu)/\sqrt2\), so $\(\hat\theta^{(2)} = \frac{X^{(1)}+X^{(2)}}{2} + \left(1 - \frac{2d-4}{\|X^{(2)}-X^{(1)}\|^2}\right)\frac{X^{(2)}-X^{(1)}}{2}, \qquad \hat\theta^{(1)} = \frac{X^{(1)}+X^{(2)}}{2} - \left(1 - \frac{2d-4}{\|X^{(2)}-X^{(1)}\|^2}\right)\frac{X^{(2)}-X^{(1)}}{2}.\)$ The total MSE for \((\theta^{(1)},\theta^{(2)})\) splits as the sum of the MSEs of \(\hat\mu\) and \(\hat\nu\): \(\hat\nu = W\) has MSE exactly \(d\), and the James–Stein estimator \(\hat\mu\) always has MSE strictly less than \(d\) (equal to \(2\) exactly when \(\mu = 0\), i.e. when \(\theta^{(1)}=\theta^{(2)}\)). So the combined estimator has MSE strictly less than \(2d\) everywhere, dropping to \(d+2\) precisely where our guess \(\theta^{(1)} \approx \theta^{(2)}\) is exactly right.

3. A nonparametric two-sample problem: Rao–Blackwellization and asymptotics

Let \(X_1,\dots,X_n \stackrel{\text{i.i.d.}}{\sim} P\) and, independently, \(Y_1,\dots,Y_n \stackrel{\text{i.i.d.}}{\sim} Q\), real-valued and with no further assumption on \(P,Q\). Two facts are given as tools: in the one-sample nonparametric model the order statistics \(S(X) = (X_{(1)},\dots,X_{(n)})\) are complete sufficient; and if \(Z_n \Rightarrow Z\), \(W_n \Rightarrow W\) with \(Z_n \perp W_n\) for every \(n\), then \((Z_n,W_n) \Rightarrow (Z,W)\) with \(Z \perp W\). Here \((S(X),S(Y))\) is (without proof) complete sufficient for the joint model.

(a) UMVU by Rao–Blackwellization. For the estimand \(g(P,Q) = \mathbb{P}_{X\sim P, Y\sim Q}(X>Y)\), start from the trivially unbiased \(\mathbf{1}\{X_1 > Y_1\}\) and Rao–Blackwellize by conditioning on the complete sufficient statistic. Conditional on \((S(X),S(Y))\), \(X_1\) and \(Y_1\) are independent uniform draws from the two order-statistic sets, so the UMVU estimator is $\(\frac{1}{n^2}\sum_{i,j=1}^n \mathbf{1}\{X_i > Y_j\}\)$ (a close relative of the Mann–Whitney statistic). Two natural-looking alternatives fail: \(\frac{1}{n}\sum_i \mathbf{1}\{X_i>Y_i\}\) is unbiased but is not a function of the sufficient statistic, so by Lehmann–Scheffé it cannot be the UMVU estimator; and \(\frac{1}{n}\sum_i \mathbf{1}\{X_{(i)}>Y_{(i)}\}\) (pairing the ordered samples) is not even unbiased. The correct estimator can equally well be written with ordered values, \(\frac{1}{n^2}\sum_{i,j}\mathbf{1}\{X_{(i)}>Y_{(j)}\}\), as long as all \(n^2\) pairs appear once.

(b) Consistency via the continuous mapping theorem. With \(\mu=\mathbb{E}_P X\), \(\nu=\mathbb{E}_Q Y > 0\), \(\sigma^2 = \mathrm{Var}_P(X)\), \(\tau^2=\mathrm{Var}_Q(Y)\) finite and positive, the law of large numbers gives \(\overline X \to \mu\), \(\overline Y \to \nu\) in probability, and \(f(x,y)=(x/y)^2\) is continuous everywhere except at \(y=0\) — which \(\overline Y\) avoids in the limit — so \(T(X,Y) = (\overline X/\overline Y)^2 \to \theta = (\mu/\nu)^2\) in probability by the continuous mapping theorem.

(c) Asymptotic normality via the delta method. The joint CLT gives $\(\sqrt n\left(\binom{\overline X_n}{\overline Y_n} - \binom{\mu}{\nu}\right) \Rightarrow N_2(0,D), \qquad D = \begin{pmatrix}\sigma^2 & 0\\ 0 & \tau^2\end{pmatrix}.\)$ The gradient of \(f(x,y)=(x/y)^2\) at \((\mu,\nu)\) (with \(\nu\ne0\)) is \(\nabla f(\mu,\nu) = (2\mu/\nu^2,\, -2\mu^2/\nu^3)\), so the delta method gives $\(\sqrt n(T-\theta) \Rightarrow N(0,\omega^2), \qquad \omega^2 = \nabla f(\mu,\nu)'D\nabla f(\mu,\nu) = 4\left(\frac{\mu^2\sigma^2}{\nu^4}+\frac{\mu^4\tau^2}{\nu^6}\right) = \frac{4}{\nu^2}\left(\theta\sigma^2+\theta^2\tau^2\right).\)$

(d) The degenerate case \(\mu=\nu=0\). Here \(Z=\sqrt n(\overline X_n,\overline Y_n) \Rightarrow N_2(0,D)\) directly (no further scaling needed), and the continuous mapping theorem still applies to \(T=(Z_1/Z_2)^2\) even though \(f\) is discontinuous at \(Z_2=0\): the relevant, slightly more general form of the theorem only needs the set of discontinuities to have measure zero under the limiting law, which is true here since \(N_2(0,D)\) puts no mass on \(\{z_2=0\}\) — unlike in part (b), where the argument instead leaned on convergence in probability to a fixed point away from the discontinuity. Writing \(Z_1=\sigma U\), \(Z_2=\tau V\) with \(U,V\) independent standard normal, $\(T = (Z_1/Z_2)^2 = \frac{\sigma^2}{\tau^2}\cdot\frac{U^2}{V^2} \Rightarrow \frac{\sigma^2}{\tau^2}F_{1,1}.\)$ A reader uneasy about invoking the relaxed continuous mapping theorem can get the same conclusion more carefully by truncating, \(T_B(X,Y) = \min(T,B)\): since \(f(x,y)=\min((x/y)^2,B)\) is continuous everywhere, \(T_B \Rightarrow \min(\sigma^2F_{1,1}/\tau^2, B)\) for every \(B\), and letting \(B\to\infty\) shows the cdf of \(T\) converges everywhere to the (continuous) limiting cdf.

4. Bayes estimation for the uniform scale family

Let \(X \sim \mathrm{Unif}[0,\theta]\), with mean \(\theta/2\) and variance \(\theta^2/12\). Recall the \(\mathrm{Pareto}(x_0,\alpha)\) density \(p_{x_0,\alpha}(x) = \alpha x_0^\alpha/x^{\alpha+1}\) for \(x \ge x_0\).

(a) A conjugate Pareto prior. With prior \(\lambda(\theta) \propto \theta^{-(\alpha+1)}\mathbf{1}\{\theta\ge\theta_0\}\) and likelihood \(p_\theta(x) = \theta^{-1}\mathbf{1}\{x\le\theta\}\), the posterior is $\(\lambda(\theta\mid x) \propto \theta^{-(\alpha+2)}\mathbf{1}\{\theta\ge\theta_0\}\mathbf{1}\{\theta\ge x\} = \theta^{-(\alpha+2)}\mathbf{1}\{\theta \ge \max(x,\theta_0)\} \propto \mathrm{Pareto}(\max(x,\theta_0),\,\alpha+1).\)$ Under squared error loss the Bayes estimator is the posterior mean, \(\hat\theta = (1+1/\alpha)\max(\theta_0, X)\).

The reason this is worth doing carefully is a genuine trap: both the uniform and the Pareto family have parameter-dependent support, so the two indicator functions cannot be dropped the way they usually can when a family's support is fixed. Writing the posterior as \(\mathrm{Pareto}(\theta_0,\alpha+1)\) — ignoring the data-dependent floor — gives a distribution that doesn't depend on \(x\) at all, which should immediately look wrong: the data must move the posterior.

(b) A polynomial prior. With \(\lambda(\theta) = 2\theta\,\mathbf{1}\{0\le\theta\le1\}\), the posterior is $\(\lambda(\theta\mid x) \propto 2\theta\cdot\mathbf{1}\{\theta\le1\}\cdot\theta^{-1}\mathbf{1}\{x\le\theta\} = 2\cdot\mathbf{1}\{x\le\theta\le1\} \propto \mathrm{Unif}[x,1]\)$ (again, a wrong answer here — \(\mathrm{Unif}[0,1]\), forgetting that the data truncates the support from below — is the same trap as in part (a)). The Bayes estimator is \((1+X)/2\), with $\(\mathrm{MSE}(\theta) = \left(\frac{1}{2}-\frac{3\theta}{4}\right)^2 + \frac{\theta^2}{48} = \frac{7}{12}\theta^2 - \frac{3}{4}\theta + \frac{1}{4},\)$ and integrating against the prior gives the Bayes risk $\(\int_0^1 2\theta\left(\frac{7}{12}\theta^2-\frac{3}{4}\theta+\frac{1}{4}\right)d\theta = \frac{7}{24}-\frac{1}{2}+\frac{1}{4} = \frac{1}{24}.\)$

(c) The minimax risk is infinite (starred). To see this, rescale part (b): take the prior \(\frac{2\theta}{B^2}\mathbf{1}\{0\le\theta\le B\}\) for \(B>0\). Writing \(Y=X/B\), \(\zeta=\theta/B\) reduces this exactly to part (b)'s problem, so its Bayes estimator is \((X+B)/2\) and its Bayes risk scales by \(B^2\): $\(\mathbb{E}\big[((X+B)/2-\theta)^2\big] = B^2\,\mathbb{E}\big[((Y+1)/2-\zeta)^2\big] = \frac{B^2}{24}.\)$ Since the Bayes risk of any prior lower-bounds the minimax risk, and \(B^2/24 \to \infty\) as \(B\to\infty\), the minimax risk for squared error loss on this problem must be infinite. This is the general pattern for showing a minimax risk is unbounded: exhibit a family of priors whose Bayes risks diverge.

(d) A scale-invariant loss. Under squared relative error loss \(L(\hat\theta,\theta) = ((\hat\theta-\theta)/\theta)^2\), restrict to linear estimators \(aX\). The risk is $\(R(\theta) = \frac{1}{\theta^2}\Big[(a\,\mathbb{E}_\theta X-\theta)^2 + a^2\mathrm{Var}_\theta(X)\Big] = \left(\frac a2-1\right)^2+\frac{a^2}{12} = \frac{a^2}{3}-a+1,\)$ which is a constant function of \(a\) alone — the \(\theta\)-dependence cancels entirely, because relative error loss combined with a pure scale family makes the risk scale-invariant. Minimizing over \(a\) gives \(a=3/2\), with constant risk \(1/4\) for every \(\theta\).

Exercises

1. Laplace scale family. With \(X_1,\dots,X_n \stackrel{\text{i.i.d.}}{\sim} \mathrm{Laplace}(0,\theta)\), \(p_\theta(x) = \frac{1}{2\theta}e^{-|x|/\theta}\) on \(\mathbb{R}\):

(a) Show \(|X_i| \sim \mathrm{Exp}(\theta)\). (b) Find a minimal sufficient statistic for the model. Is it complete? (c) Find the MLE for \(\theta\) and its asymptotic distribution. (d) Show the estimator from (c) is unbiased. Does it attain the Cramér–Rao lower bound? (e) Now suppose \(X_i \sim \mathrm{Laplace}(0,\theta_0(1-\delta)^i)\) for \(i=1,\dots,n\), with \(\theta_0\) known. Propose a score test of \(H_0:\delta=0\) against \(H_1:\delta>0\), with an explicit statistic and an asymptotic cutoff. (f) (Starred.) Now suppose \(\theta_0\) is also unknown. Modify the test from (e) so that it has finite-sample control of the Type I error rate, explaining how you would find the cutoff without knowing \(\theta_0\).

2. Multivariate normal means. Let \(X^{(i)} \stackrel{\text{ind.}}{\sim} N_d(\theta^{(i)},\sigma^2 I_d)\) for \(i=1,2\), \(d\ge3\).

(a) With \(\sigma^2\) known, propose a test of \(H_0:\theta^{(1)}=\theta^{(2)}\) against \(\theta^{(1)}\ne\theta^{(2)}\), with a cutoff in terms of a \(\chi^2\) quantile. (b) With \(\sigma^2\) unknown and \(\theta^{(2)}_j=\theta^{(1)}_j+\delta\) for all \(j\) (a common shift), propose a finite-sample test of \(H_0:\delta=0\) against \(\delta\ne0\). (c) Under the same assumptions, give a confidence interval for \(\delta\). (d) (Starred.) With \(\theta^{(1)},\theta^{(2)}\) unrestricted and \(\sigma^2=1\), and a belief that \(\theta^{(1)}\approx\theta^{(2)}\) without further information, propose an estimator of \((\theta^{(1)},\theta^{(2)})\) with MSE less than \(2d\) everywhere, but MSE \(d+2\) whenever \(\theta^{(1)}=\theta^{(2)}\).

3. A nonparametric two-sample problem. Let \(X_1,\dots,X_n \stackrel{\text{i.i.d.}}{\sim} P\) and, independently, \(Y_1,\dots,Y_n \stackrel{\text{i.i.d.}}{\sim} Q\), both real-valued, with \((S(X),S(Y))\) complete sufficient for the joint model.

(a) Find the UMVU estimator of \(g(P,Q)=\mathbb{P}_{X\sim P,Y\sim Q}(X>Y)\) and justify its optimality. (b) With \(\mu=\mathbb{E}_PX\), \(\nu=\mathbb{E}_QY>0\), \(\sigma^2=\mathrm{Var}_P(X)\), \(\tau^2=\mathrm{Var}_Q(Y)\) finite and positive, show \(T(X,Y)=(\overline X/\overline Y)^2\) is consistent for \(\theta=(\mu/\nu)^2\). (c) Give the asymptotic distribution of \(T\), appropriately normalized, with parameters expressed in terms of \(\mu,\nu,\sigma^2,\tau^2,\theta\). (d) (Starred.) If \(\mu=\nu=0\), give the (appropriately normalized, if necessary) asymptotic distribution of \(T\), and justify the argument.

4. Bayes estimation for the uniform scale family. Let \(X\sim\mathrm{Unif}[0,\theta]\). Assume squared error loss for parts (a)–(c).

(a) Show \(\theta\sim\mathrm{Pareto}(\theta_0,\alpha)\) is conjugate, and find the posterior and Bayes estimator. (b) Repeat for the prior \(\lambda(\theta)=2\theta\,\mathbf{1}\{0\le\theta\le1\}\): find the Bayes estimator and the Bayes risk. (c) (Starred.) Is the minimax risk for this problem finite? Prove it is infinite, or exhibit a finite upper bound. (Hint: consider a version of the problem with \(\theta\) bounded above by some \(B>0\).) (d) Under squared relative error loss \(L(\hat\theta,\theta)=((\hat\theta-\theta)/\theta)^2\), find the best estimator of the form \(aX\) (\(a>0\)): the minimizing \(a\) and the resulting risk as a function of \(\theta\).

Sources

All of this chapter is drawn from the Fall 2023 STAT 210A (UC Berkeley, Prof. Will Fithian) final examination question booklet, which is a combined problem-and-solution document (the exam booklet itself, converted together with its solutions):

  • Title page and exam instructions: 01-final-examination-question-booklet.md
  • Problem 1, Laplace location family: 02-1-laplace-location-family-24-points-4-points-part.md
  • Problem 2, multivariate normal means: 03-2-multivariate-normal-means-20-points-5-points-part.md
  • Problem 3, nonparametric two-sample problem: 04-3-nonparametric-two-sample-problem-20-points-5-points-part.md
  • Problem 4, Bayes estimation for the uniform scale family: 05-4-bayes-estimation-for-uniform-scale-family-20-points-5-poin.md

all under docs/statistics/berkeley/stat210a/fall-2024/old-exams/solution2023/ in the knowledge-base-library repository. Byte-identical copies of the same booklet, differing only in which course-instance directory they are filed under, also appear under the fall-2025, fall-2025/units, and fall-2026 old-exams/solution2023/ directories; only the fall-2024 copy is cited above.

The source markdown carries its own provenance note worth repeating here: it was reconstructed by a model from a PDF with no extractable text layer, the prose is a paraphrase in places, and every equation in it is unverified against the original PDF. This chapter reorganizes and explains that material but does not independently re-derive or check it against the source PDF; treat the mathematics here with the same caveat the source itself carries.

No slides or lecture transcript were supplied for this chapter — the entire input is the exam booklet listed above.


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