This is a special case of homework problem 8-4 in the notes. The problem statement says that
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The distribution of T is symmetric about zero, so E(T) = 0 when the
expectation exists (which the problem says to assume). Thus by linearity
of expectation
.
Same as part (a). When a distribution has a center of symmetry, then
the center of symmetry is the the median as well the mean when the mean exists.
Thus
is also the posterior median.
The likelihood is
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The mean of a
distribution is a / b (equation (7) on
p. 174 in Lindgren). Hence the mean here is
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Part (a) of this problem is essentially the same as Problem 3 on the first midterm. The p. d. f. in this problem is obtained from the p. d. f. in that problem by the transformation y = 1 / x. The MLE in that problem was found to be
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The joint p. d. f. is
Hence the log likelihood is
To simplify notation, define

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We have two options for calculating Fisher information. We can calculate
the variance of
, or we can calculate the negative expectation
of the second derivative of the log likelihood
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The general formula for a 95% confidence interval for the parameter based on the asymptotic distribution of the MLE is

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An exact C. I. is derived using the pivotal quantity having the exact sampling distribution
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An equal-tailed confidence interval uses points a* and b*
such that
. The confidence interval
is the interval of
satisfying
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Looking in Table Vb in the row for 4 d. f. and in the columns for 2.5% and 97.5%, we find a* = 0.484 and b* = 11.1.
Since
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The problem did not explicitly ask for equal-tailed confidence intervals.
The problem could have been answered with a semi-infinite interval like
Example 8.9a in Lindgren, i. e., what you get when you take a* = 0 and
b* = 9.45 (from the 95% column) or when you take a* = 0.711 (from the
5% column) and
. The first choice gives an exact 95%
C. I. for
of
, and the second choice gives an
exact 95% C. I. for
of (0, 301).
There are zillions of consistent estimators. The question is to find one.
The MLE is consistent but impossible to find in closed form, because
the score function involves derivatives of gamma functions. Thus we turn
to the method of moments. The mean and variance of the
distribution are
(p. 176 in Lindgren). Plugging
gives
The first equation is useless because it does not contain
.Solving the second for
gives
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