Proof of Radon-Nikodym theorem
Theorem (Radon-Nikodym). Suppose Ω is a nonempty set andA aσ-field on it. Supposeµand ν are σ-finite measures on (Ω,A) such that for all A∈A, µ(A) = 0 impliesν(A) = 0. Then
• There exists z : Ω→[0,∞) measurable such that for all A∈A, ν(A) =R
Az dµ.
• Such a z is unique upto a.e. equality (w.r.t.µ).
• z is integrable w.r.t. µif and only if ν is a finite measure.
Proof. Assuming we have obtained the z, it is easy to see that z is integrable if and only ifν is a finite measure, since ν(Ω) =R
z dµ.
Uniqueness
We show uniqueness first. Suppose there are two z1, z2 : Ω → [0,∞) such that for all A ∈ A, R
Az1 dµ=ν(A) =R
Az2 dµ. We would like to say R
Az1 dµ−R
Az2 dµ= 0, but both the integrals might be ∞. Both µ and ν are σ-finite. Let C be a countable partition of Ω such that for all C ∈ C, µ(C) < ∞ and ν(C) <∞ (to obtain this we can take such a partition for µ, and such a partition for ν, and take pairwise intersections). Fix a C ∈ C. Let
B =C∩ {ω :z1(ω)−z2(ω)>0}
Note that 1B(z1−z2) = 1C(z1−z2)+(evaluate both sides atω: forω /∈C, both are 0; forω∈C\B, LHS is 0 and since (z1 −z2)(ω) ≤ 0, RHS is 0; for ω ∈ B both side are z1(ω)−z2(ω)). ν(B) = R 1Bz1dµ=R
1Bz2dµ. Sinceν(B)≤ν(C)<∞, it is meaningful to considerR
1Bz1dµ−R
1Bz2dµ.
0 = Z
1Bz1 dµ− Z
1Bz2 dµ
= Z
1B(z1−z2) dµ
= Z
1C(z1−z2)+ dµ
If the integral of a nonnegative function is 0, it must be 0 almost everywhere. Applying to the above:
µ({ω :ω ∈C and z1(ω)−z2(ω)>0}) = 0
We can interchange the roles of z1 and z2 in the above argument. Combining the two, we get µ({ω :ω ∈C and z1(ω)−z2(ω)6= 0}) = 0
This holds for all C∈ C. SinceC is countable, and a countable union of null sets is a null set, µ({ω :z1(ω)6=z2(ω)}) = 0
This proves that the z promised in the theorem (if it exists) is unique upto a.e. (w.r.t.µ) equality.
Existence
We now show the existence of such a z. We reduce the general case to the case when both µand ν are finite, and then show existence for the finite case.
Reduction to the finite measure case
Suppose we know the Radon-Nikodym theorem holds for the case when the measures involved are finite. In general, assume µ and ν are σ-finite, and let C be a countable partition of Ω such that for all C ∈ C,µ(C) and ν(C) are finite. Define finite measures µC and νC for all C ∈ C,
µC(A) = µ(C∩A), νC(A) =ν(C∩A)
If µC(A) = 0, then νC(A) = 0. Using the finite-measure case of the theorem, let zC : Ω →[0,∞) be such that for all A∈A and C∈ C,
νC(A) = Z
A
zC dµC
zC and zC1C differ at most on Ω\C, which has 0 µC measure. So we can replace zC by zC1C, and so assume that for ω /∈ C, zC(ω) = 0. Define z : Ω → [0,∞), by requiring that z|C = (zC)|C (that is, for ω ∈ C, z(ω) = zC(ω)). z can also be described as P
C∈CzC - this shows that z is measurable.
If g : Ω→[0,∞) is 0 outside C, then R
g dµ=R
g dµC. This can be proven as usual by proving it for simple functions and then for all nonnegative measurable functions. This fact is applied to zC in what follows. For anyA ∈A,
ν(A) =X
C∈C
ν(A∩C)
=X
C∈C
νC(A)
=X
C∈C
Z
A
zC dµC
=X
C∈C
Z
A
zC dµ
= Z
A
X
C∈C
zC dµ (by taking partial sums; MCT)
= Z
A
z dµ
It remains to prove the theorem for the finite measure case:
Finite measures - getting hold of the z:
Now assume µand ν are finite measures. Let C =
f : (f : Ω→[0,∞]R¯),∀A∈A(R
Af dµ≤ν(A))
We want to identify f such that equality holds, that is, for all A∈A, R
Af dµ=ν(A).
C is nonempty, because the zero function belongs toC. Intuitively, we want to choose the “largest”
function in C as a candidate for our z. Does such a “largest” function exist? We observe some properties of C first:
• Iff, g ∈C, thenf∨g (which is the pointwise maximum off and g) belongs to C. Take any A ∈ A. We apply the condition defining C to the sets A1 := A∩ {ω : f(ω) ≥ g(ω)} and A2 :=A∩ {ω :f(ω)< g(ω)}:
Z
A1
f ≤ν(A1), Z
A2
g ≤ν(A2)
Note thatf1A1 = (f∨g)1A1 andg1A2 = (f∨g)1A2. Substituting in the above equations and adding them, we get
Z
A
(f ∨g)≤ν(A)
• Suppose {fn}∞n=1 is an increasing sequence in C. Let f be their supremum (equivalently limit). Then f ∈C: take any A ∈A. {fn1A}∞n=1 increases to f1A, and so by the monotone convergence theorem the corresponding limit with integrals holds. Since eachR
fn1A≤ν(A), we have R
f1A≤ν(A).
We identify the “largest” function in C by considering the function with the largest integral. For all f ∈C, R
f dµ≤ν(Ω)<∞. Let
α= supn
R f dµ :f ∈Co
0 ≤α ≤ν(Ω). In particular, α 6=∞. Let {fn}∞n=1 be a sequence from C such that R
fn dµ ∞
n=1
converges to α (this can be done because of the supremum definition of α). Consider the partial maxima of {fn}∞n=1, that is, define {gn}∞n=1 by
gn = max{f1, f2, . . . , fn} We know that gn ∈ C, so R
gn dµ ≤ α. Also, fn ≤ gn, so R
fn dµ ≤ R
gn dµ ≤ α. Thus limn→∞
R gn dµ = α. {gn}∞n=1 is an increasing sequence; let z = limn→∞gn. By the monotone convergence theorem, R
z dµ=α. Since z is integrable, z is finite almost everywhere. We modify z on a set of measure 0 suitably so thatz never takes the value∞. Thisz is our “largest” function in C, as we show now:
Let g ∈ C. We will show that g ≤ z a.e. (w.r.t µ). Let A = {ω : g(ω) > z(ω)}. Let z∨g = h.
h∈C. A={ω:h(ω)> z(ω)}={ω :h(ω)−z(ω)>0}. h ≥z;R
h dµ≥R
z dµ=α, so R
h=α.
h−z is a nonnegative function whose µintegral is 0, so h−z is 0 almost everywhere. µ(A) = 0.
g ≤z almost everywhere (w.r.t µ).
Finite measures - showing that the z works Define λ:A →[0,∞),
λ(A) = ν(A)− Z
A
z dµ
Note that this is well-defined, that is, the expression on the RHS indeed belongs to [0,∞). λ is a measure: clearly λ(∅) = 0. LetC ⊆A be a countable collection of disjoint sets.
X
C∈C
ν(C) +X
C∈C
Z
C
z dµ =ν[ C
+ Z
SC
z dµ <∞
Since the relevant series is absolutely convergent, we can rearrange terms, and λ[
C
=ν[
C
− Z
SC
z dµ =X
C∈C
ν(C)−X
C∈C
Z
C
z dµ=X
C∈C
ν(C)− Z
C
z dµ
=X
C∈C
λ(C)
λ is a measure. We want to show that λ is the zero measure, and then we will be done.
If for all A ∈ A and all k ∈ N, λ(A) ≤ 1kµ(A) then since µ(A) is finite, λ(A) = 0, and we are done. So there exists A ∈A and k ∈ N such that λ(A)− 1kµ(A)> 0. Fix such an A and k. We will derive a contradiction.
Call a set Z ∈A to be good if the following two conditions hold:
• λ(Z)− 1kµ(Z)>0.
• For all B ⊆Z with B ∈A, λ(B)− 1kµ(B)≥0.
The first condition implies that a good set Z must haveµ(Z)>0: otherwise ifµ(Z) = 0, then by the hypothesis, ν(Z) = 0, and soλ(Z) = 0. A satisfies the first condition, but need not satisfy the second condition.
We will identify a good set - A itself may not be a good set, but we can “scrape off” some parts of it to get a good set. Once we identify a good set Z, we will use the function z +k11Z to get a contradiction.
Let A0 =A. Let β0 = inf{λ(B)− 1kµ(B) : B ⊆A, B ∈A}. If β0 ≥0, then A itself is a good set.
So assume β0 <0. β0 cannot be −∞, since it is at least −(ν(Ω) +R
z dµ+1kµ(Ω)). Pick B0 ⊆A0 such that
λ(B0)− 1
kµ(B0)< 1 2β0 Put A1 =A\B0.
λ(A1)− 1kµ(A1) = λ(A)−λ(B0)
− k1µ(A)− 1kµ(B0)
≥λ(A)−k1µ(A)>0 (because λ(B0)− 1kµ(B0)< 12β0 <0.)
An important observation is this: if B ⊆A1, thenλ(B)−k1µ(B)≥ 12β0. Otherwise, we could take a B which violates this, and B∪B0 would violate the infimum definition of β0.
If A1 is a good set, we have found a good set. Otherwise, repeat with A1 what we did with A0. The above observation says that theβ1so obtained will satisfyβ1 ≥ 12β0. Inductively, we construct a sequences of sets {An}∞n=1 and {Bn}∞n=1, and a sequence of real numbers {βn}∞n=1, such that the following holds: some An is good, or for all n∈N,
• Bn⊆An.
• An+1 =An\Bn.
• βn = inf
λ(B)− 1kµ(B) :B ⊆An, B ∈A ,βn <0.
• λ(An+1)− 1kµ(An+1)≥λ(An)− 1kµ(An).
• βn+1 ≥ 12βn.
This immediately implies that for all n,βn ≥ 21nβ0 and λ(An)− 1kµ(An)≥λ(A)− 1kµ(A)>0.
If no An was good, define A∞ =T
n∈NAn. Since λ and µare finite measures, λ(A∞) = lim
n→∞λ(An) and µ(A∞) = lim
n→∞µ(An)
So λ(A∞) − 1kµ(A∞) ≥ λ(A)− 1kµ(A) > 0. If B ⊆ A∞ and B ∈ A, then since B ⊆ An, λ(B)−k1µ(B)≥ 21nβ0. Since this holds for alln,λ(B)−1kµ(B)≥0. A∞ is a good set! If someAn
was good, let A∞ be that good set.
We will show that z+ 1k1A∞ ∈C. For any S ∈A, if S ⊆Ω\A∞, then Z
S
z+ 1
k1A∞
dµ=
Z
S
z dµ ≤ν(S)
If S ⊆A∞, then R
S z+1k1A∞
dµ=R
Sz dµ+ 1kµ(S)
≤R
Sz dµ+λ(S) (since A∞ is a good set)
=ν(S) (by definition of λ)
For general S, we just combine the part ofS in A and the part in Ω\A:
Z
S
z+1
k1A∞
dµ= Z
S∩A
z+1
k1A∞
dµ+
Z
S\A
z+ 1
k1A∞
dµ≤ν(S∩A)+ν(S\A) =ν(S)
We have shown that z+ 1k1A∞ ∈ C. Since A∞ is a good set, µ(A∞) >0. It is not the case that z+ 1k1A∞ ≤z a.e. (w.r.t. µ), which contradicts what we have shown earlier.
λ must be the zero measure, and so for all D∈A, ν(D) =
Z
D
z dµ