|
Size: 1453
Comment: More notes
|
← Revision 4 as of 2026-07-30 20:12:48 ⇥
Size: 1712
Comment: Term
|
| Deletions are marked like this. | Additions are marked like this. |
| Line 28: | Line 28: |
| The convention for arithmetic with ∞ in measure spaces is that: * ''x + ∞ = ∞'' for all ''x ∈ [0,∞]'' * ''x * ∞ = ∞'' for all ''x ∈ (0,∞]'' * ''0 * ∞ = 0'' |
|
| Line 30: | Line 35: |
| * additivity * for a [[Analysis/Cardinality|countable]] set of ''n'' elements, requiring that each is disjoint (i.e. ''A,,i,, ∩ A,,j,, = Ø, i != j''): {{attachment:countable.svg}} * for an infinite set: {{attachment:infinite.svg}} |
* '''σ additivity''': additivity for finite and [[Analysis/Cardinality|countably]] infinite elements, but not infinite elements * in the finite case, requiring that each is disjoint (i.e. ''A,,i,, ∩ A,,j,, = Ø, i != j''): {{attachment:countable.svg}} * in the countable case: {{attachment:infinite.svg}} |
Measure Space
Contents
Introduction
To motivate a theory of measures:
"[I]n one dimension, the intervals A := [0, 1] and B := [0, 2] are in one-to-one correspondence (using the bijection x -> 2x from A to B), but of course B is twice as long as A. So one can disassemble A into an uncountable number of points and reassemble them to form a set of twice the length." (p3, An Introduction to Measure Theory, Terence Tao)
Description
A measure space is a triple (Ω, 𝒜, μ), composed of:
a sample space Ω
a σ algebra 𝒜
Note that the double (Ω, 𝒜 ) is sometimes called a measurable space.
a measure μ : 𝒜 -> [0,∞]
Note that [0,∞] is shorthand for the more formally correct [0,∞) ∪ {∞}.
The convention for arithmetic with ∞ in measure spaces is that:
x + ∞ = ∞ for all x ∈ [0,∞]
x * ∞ = ∞ for all x ∈ (0,∞]
0 * ∞ = 0
As for a measure, this is a map from 𝒜 to non-negative real numbers. It must satisfy two conditions:
μ(Ø) = 0
σ additivity: additivity for finite and countably infinite elements, but not infinite elements
in the finite case, requiring that each is disjoint (i.e. Ai ∩ Aj = Ø, i != j):
in the countable case:
It should be clear that these conditions are the reason for conditions 1 and 3 on the definition of a σ algebra.
