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Radon-Nikodym Theorem

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Theorem
MeasureTheory

Motivation

Let (X,F)(X,\mathcal{F}) be a measurable space. Let μ\mu be a measure on F\mathcal{F}. Let fL1(X,F,μ)f\in L^{1}(X,\mathcal{F},\mu), define a new measure ν\nu as ν(E)=Efdμ\nu(E)=\int\limits _{E}f \, d\mu we see that ν\nu is a finite measure. Now we would like to do the reverse, i.e. given two measures μ,ν\mu,\nu where νμ\nu\ll \mu can we find a ff s.t. the above holds?

Let (X,F,μ)(X,\mathcal{F},\mu) be a measure space, with μ\mu as a finite signed measure. Let ν\nu be a measure on (X,F)(X,\mathcal{F}) and assume νμ\nu\ll\mu (i.e. ν\nu absolutely continuous w.r.t μ\mu). Then !fL1(X,F,μ)\exists!f\in L^{1}(X,\mathcal{F},\mu) such that ν(A)=Afdμ\nu(A)=\int\limits _{A}f \, d\mu AF\forall A\in\mathcal{F}.

Let (X,M)(X,\mathscr{M}) be a measurable space and μ\mu a σ-finite measure on M\mathscr{M}. Let ν\nu be a finite measure on M\mathscr{M}. 1. There exists a unique pair of measures νa,νs\nu_{a},\nu_{s} on M\mathscr{M} such that: 1. ν=νa+νs\nu=\nu_{a}+\nu_{s} 2. νaμ\nu_{a}\ll \mu 3. νsμ\nu_{s}\perp \mu, (i.e. νs,μ\nu_{s},\mu are Mutually Singular) 2. hL1(X,M,μ)\exists h\in L^{1}(X,\mathscr{M},\mu) such that νa(E)=EhdμEM\nu_{a}(E)=\int\limits _{E}h \, d\mu\quad \forall E\in\mathscr{M}

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