Notes:The set of all mu*-measurable sets is a ring
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In Measure Theory Halmos does something weird for section 11, theorem B. I have yet to "crack" what he's doing, and this is the point of this page.
Halmos' theorem:
Section 11 - Theorem B - page 46:
- If μ∗:H→ˉR≥0 is an outer-measure on a hereditary sigma-ring, H and if S is the set of all μ∗-measurable sets then S is a sigma-ring.
- Furthermore, if A∈H and if (En)∞n=1⊆S is a sequence of pair-wise disjoint sets, and E:=⋃∞n=1En then:
- μ∗(A∩E)=∞∑n=1μ∗(A∩En)
- μ∗(A∩E)=∞∑n=1μ∗(A∩En)
Context:
- The previous theorem proved was that S is a ring of sets.
- I have proved that μ∗|S - the restriction (function) of μ∗ to S - is a pre-measure.
His proof
Step | Comment |
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Notice we have:
μ∗(A∩(E1∪E2))=μ∗(A∩E1)+μ∗(A∩E2) |
As A∩(E1∪E2)⊆A∩E1 and A∩(E2∪E2)⊆A∩E2 we see:
(This requires that they are disjoint for the subtraction side to be true) We could just as well have used E2 to split. |
It follows by induction that:
For every n∈N≥0 |
Agreed |
Define:
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"Then it follows from theorem A" that:
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First note that:
Next note that A−Fn⊇A−Fm for m≥n, so:
Thus:
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"Since it is true for every n we obtain":
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Unsure:
(See details below) |
Details
I am completely happy with:
- μ∗(A∩⋃ni=1Ai)=∑ni=1μ∗(A∩Ei)
- μ∗(A−E)≤μ∗(A−⋃ni=1Ai)
- μ∗(A)=μ∗(A∩Fn)+μ∗(A−Fn) (this is okay because S is a ring, thus the finite union, Fn∈S.)
- This is: μ∗(A)=μ∗(A∩⋃ni=1Ei)+μ∗(A−⋃ni=1Ei) by definition of Fn.
Combining these we see:
- μ∗(A)=μ∗(A∩Fn)+μ∗(A−Fn)≥μ∗(A∩Fn)+μ∗(A−E)=∑ni=1μ∗(A∩Ei)+μ∗(A−E)
I've also consulted Measures Integrals and Martingales, it has the same thing in it. Both books say (and require):
- ∞∑n=1μ∗(A∩En)≥μ∗(A∩E)
I could believe ∀m∈N[∑mi=1μ∗(A∩En)≤μ∗(A∩E)] (by monotonicity of the outer-measure) but I cannot justify this.
I am also nervous about: ∀m∈N[μ∗(A)≥∑mi=1μ∗(A∩Ei)+μ∗(A−E)]⟹μ∗(A)≥∑∞n=1μ∗(A∩En)+μ∗(A−E) however:
- The sequence ((no content) )∞n=1 is monotonically increasing, and it is bounded above (if μ∗(A) is finite), thus is finite, and there's a similar case to be made in the infinite case. I don't know how to jump from the finite to the infinite case.