STA 6466: Assignments
- Assignment 1 (Due Aug 30). The statements of the following
problems can be found here.
- To turn in: Billingsley, exercises 2.5(b), 2.9, 2.11.
- Suggested: Billingsley, exercises 2.3, 2.4, 2.7, 2.8,
2.10.
- Assignment 2 (Due Sep 6).
- To turn in: Billingsley, exercises 2.13, 10.2.
- Suggested: Billingsley, exercises 2.17, 10.1, 10.3.
- Assignment 3 (Due Sep 13).
- To turn in: Billingsley, exercises 3.11,
3.12(b–c).
- Suggested: Billingsley, exercises 3.13.
- Assignment 4 (Due Sep 20).
- To turn in: Billingsley, exercises 2.19, 12.9
(hints)
- Assignment 5 (Due Sep 27).
- To turn in: Billingsley, exercises 13.1, 13.8.
- Hint for 13.8: Show that {x: f(x) < t}
is open for all real t. If your solution is more than
just a few lines, you're working too hard. BTW, where
Billingsley says "for each ε" he means "for
each ε > 0."
- Suggested: Billingsley, exercises 12.1, 12.11, 13.6.
- Hints for 12.1: For the linear (i.e., 1-dimensional)
case, consider the function f(x) = μ((0, x]) and
use Cauchy's equation from Appendix A20 of
Billingsley.
The k-dimensional case can be done using induction
on k. To go from k to k+1 dimensions, let B be a
fixed linear Borel set, and consider μ(A x B), as
A varies over the k-dimensional Borel sets. You can
show that this defines a translation invariant
measure on the k-dimensional Borel sets, and by the
induction hypothesis, this measure must be a
constant multiple of k-dimensional Lebesgue measure,
with the constant α(B) possibly depending on
B.
Next show that as B varies over the linear Borel
sets, α(B) defines a translation invariant
measure, which implies that α(B) is a constant
multiple of Lebesgue measure on the real line. For
this note that α(B) = μ(A x B) where A is a
k-dimensional Borel set with Lebesgue measure 1 (you
should be able to write down at least one such set).
Now put these two pieces together to show that
the μ-measure of a k+1 dimensional rectangle is a
constant multiple of its volume, and invoke the
uniqueness theorem for σ-finite measures.
- Note: In exercise 12.11, the claim that C supports
the corresponding measure is false without the
additional hypothesis that G is continuous, so you
must assume continuity for (only) this part of the
problem; try to find a counterexample in the
discontinuous case.
- Assignment 6 (Due Oct 4)
- To turn in: Billingsley, exercises 13.9, 13.10.
- Suggested: Billingsley, exercises 13.11, 13.14,
14.1, 14.3, 14.4.
- In problem 14.3, φ represents the quantile
function of F. You should probably use the notation
from class for this instead, i.e, F−1
instead of φ.
- Assignment 7 (Due by noon on Oct 19).
- To turn in: Billingsley, exercises 16.4, 16.8.
- Suggested: Billingsley, exercises 16.2.
- Assignment 8 (Due by noon on Oct 26).
- To turn in: Billingsley, exercises 17.6, 17.8.
- Hint for 17.8: Use symmetry and Billingsley's
equation (17.8) for the first part.
- Suggested: Billingsley, exercises 17.5, 17.7.
- Assignment 9 (Due Nov 1)
- To turn in: Billingsley, exercises 32.6, 32.9.
- In part (a) of exercise 32.6, because dν/dρ
is uniquely defined only up to ρ-a.e. equality,
the statement dν/dρ = (dν/dμ) ×
(dμ/dρ) should be interpreted to mean that the
right-hand side is a "version" of dν/dρ. The
easiest and most clearly correct way to show this is
to show that the right-hand side satisfies the
operational definition of dν/dρ, i.e., that it
is indeed a density for ν with respect to ρ.
In fact, this must hold regardless of the versions of
dν/dμ and dμ/dρ used in constructing the
right-hand side, though this does not really affect
the proof in any way. Similar comments apply to parts
(b) and (c).
- In problem 32.9, assume only that ν and
ν0 are σ-finite. There is no need
to assume that μ and ν are finite. Note,
however, that if ν is finite then so is
ν0, whereas σ-finiteness of ν
does not imply σ-finiteness of ν0.
Thus we must also assume that ν0 is
σ-finite in order to generalize the result to
σ-finite ν.
- Suggested: Billingsley, exercises 32.10.
- In problem 32.10, you need only assume that ν and
νn are σ-finite. There is no need
to assume that the measures involved are finite.
- Assignment 10 (Due Nov 16)
- To turn in: Billingsley, exercises 18.6, 18.13, 32.5.
- Problem 18.6 is straightforward once you prove that
"the set on the right is measurable" (meaning that it
is contained in the product σ-field). I guess
the easiest way to do this is to first show that the
functions g(ω, y) = y and h(ω, y) =
f(ω) are measurable from the product space into
the reals.
- In problem 32.5, it is very easy to see that the
"σ-field of vertical strips" is a
sub-σ-field of the "planar" (i.e.,
two-dimensional) Borel sets. It is then immediate
that the restriction of planar Lebesgue measure to
this σ-field is indeed a measure. You can just
say this without further elaboration. It is also easy
to show that ν, as defined, is a measure on the
σ-field of vertical strips, so please do not
write more than a few lines about this either. (Of
course you should ask me about any of this that is not
completely clear to you).
Having said all that, once you write down the
measures assigned by μ and ν to a typical set A
× R in the σ-field of vertical strips, it
will be easy to see that ν ≪ μ. To
finish the problem, it is helpful to know that in
order for a real-valued function f on the plane to be
measurable with respect to the σ-field of
vertical strips, the value of f(x,y) must depend only
on x, or more precisely, f must have the form f(x,y) =
g(x), where g is Borel measurable. Of course if you
use this fact, you should prove it.
- Suggested: Billingsley, exercises 18.1, 18.2, 18.3,
18.4, 18.8, 18.10, 18.14, and
this
problem.
- Problem 18.2 is fairly complicated. Billingsley's
hint lays out the basic approach. Near the end you
need to recognize that the σ-field generated by
a countable partition of a space consists of the class
of all unions of sets in the partition (together with
the empty set), which is easy to show.
- For problem 18.3, Billingsley's hint together with
problem 18.1 makes the problem easy once you recall
that the nonmeasurable set contructed in class is not
only not a Borel set, it is not Lebesgue measurable
either.
- Assignment 11 (Due Nov 29): Turn in problems 4 and 5 from
this sheet.