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Total Variation 📂Measure Theory

Total Variation

Definition1

A total variation ν| \nu | of a signed measure ν\nu on a measurable space (X,E)(X, \mathcal{E}) is defined as follows.

ν=ν++ν |\nu |= \nu^{+} +\nu^{-}

Here, ν=ν+ν\nu=\nu^{+}-\nu^{-} is the Jordan decomposition of ν\nu.

Explanation

ν+\nu^{+} and ν\nu^{-} are called the positive variation and negative variation of ν\nu, respectively. The Jordan decomposition and the total variation for a measure are exactly the same as the method of expressing any function as two non-negative functions. The following holds for the total variation ν|\nu|.

Theorem 1

Let’s say EEE \in \mathcal{E}. Then, the two propositions below are equivalent.

  • (a) EE is ν\nu-null.
  • (b) EE is ν|\nu|-null.

Proof

  • (a)     \implies (b)

    If EE is ν\nu-null, let’s say X=PNX=P\cup N is a partition of ν\nu. Then, by assumption, the following holds for all FEF\subset E, FEF\in \mathcal{E}.

    ν+(F)=ν(FP)=0ν(F)=ν(FN)=0 \begin{align*} \nu^{+}(F) &= \nu (F \cap P)=0 \\ \nu^{-}(F) &= \nu (F \cap N)=0 \end{align*}

    Therefore, the below equation is valid.

    ν(F)=ν+(F)+ν(F)=0,FE | \nu | (F)= \nu^{+}(F) + \nu^{-}(F)=0,\quad \forall F\subset E

    Thus, EE is ν| \nu |-null.

  • (b)     \implies (a)

    If EE is ν| \nu |-null, then the following holds for all FEF\subset E, FEF\in \mathcal{E}.

    ν(F)=ν+(F)+ν(F)=0 | \nu | (F)=\nu^{+} (F) +\nu ^- (F)=0

    However, since ν+\nu^{+}, ν\nu^{-} are mutually singular, for the above equation to hold, necessarily ν+(F)=0\nu^{+} (F)=0, ν(F)=0\nu^{-} (F)=0 must be true. Therefore, we obtain the following.

    ν(F)=ν+(F)ν(F)=0,FE \nu (F) = \nu^{+} (F) - \nu^{-} (F)=0,\quad \forall F\subset E

    Thus, EE is ν\nu-null.


It can be seen in the proof process that the equivalent condition is expanded as follows.

  • (a) EE is ν\nu -null.
  • (b) EE is ν|\nu| -null.
  • (b’) EE is ν+\nu^{+} -null, ν\nu^{-} -null.

Theorem 2

For two signed measures ν\nu, μ\mu, the conditions below are all equivalent.

  • (c) νμ\nu \perp \mu
  • (d) ν+μ\nu^{+} \perp \mu and νμ\nu^{-} \perp \mu
  • (e) νμ|\nu| \perp \mu

Proof

  • (c)     \implies (d)

    By assumption, there exist EF=XE \cup F =X, EF=E \cap F=\varnothing where EE is ν\nu-null, and FF is μ\mu-null. Showing that EE is ν+\nu^{+}-null, ν\nu^{-}-null according to the definition of mutually singular completes the proof. Since Theorem 1 establishes that if EE is ν\nu-null, it is also ν+\nu^{+}-null, ν\nu^{-}-null, the following holds.

    ν+μandνμ \nu^{+} \perp \mu \quad \text{and} \quad \nu^{-} \perp \mu

  • (d)     \implies (e)

    By assumption, E+E_+ is ν+\nu^{+}-null, and there exist E+F+=XE_+ \cup F_+ =X, E+F+=E_+ \cap F_+=\varnothing where FF is μ\mu-null. Also, EE_- is ν\nu^{-}-null, and there exist EF=XE_- \cup F_- =X, EF=E_- \cap F_-=\varnothing where FF is μ\mu-null. Now, let’s define the set A, B1, B2, B3A,\ B_{1},\ B_2,\ B_{3} as follows.

    A:=E+E,B1:=E+FB2:=F+F,B3:=EF+ A:= E_+ \cap E_-,\quad B_{1}:=E_+ \cap F_- \\ B_2:=F_+ \cap F_- ,\quad B_{3}:=E_- \cap F_+

    Then, the four sets are mutually exclusive and satisfy the following.

    AB1B2B3=X A\cup B_{1} \cup B_2 \cup B_{3} =X

    And AA is ν+\nu^{+}-null and ν\nu^{-}-null. Therefore, AA is ν| \nu |-null. Also, for all jj, BjB_{j} is μ\mu-null. Let’s say B=BjB=\cup B_{j}. Then AB=XA\cup B=X, AB=A \cap B=\varnothing and since AA is ν| \nu |-null, BB is μ\mu-null, the following is valid.

    νμ | \nu| \perp \mu

  • (e)     \implies (c)

    Since $**

    가정에 의해 EEν| \nu |-null이고, FFμ\mu-null인 EF=XE \cup F =X, EF=E \cap F=\varnothing가 존재한다. 정리 1 에 의해 EEν| \nu |-null이면 ν\nu-null" also holds, the proof is complete.


  1. Gerald B. Folland, Real Analysis: Modern Techniques and Their Applications (2nd Edition, 1999), p ↩︎