Let $(\Omega,\mathscr{F}, P)$ be a probability space, let $\nu$ be a finite measure on $\mathscr{F}$, and let $\mathscr{F}_{1}$, $\mathscr{F}_{2}$,... be a non-decreasing sequence of $\sigma$-fields in $\mathscr{F}$. Suppose that $P$ dominates $\nu$ when both are restricted to $\mathscr{F}_{n}$. There is then a density or Radon-Nikodym derivative $X_{n}$ of $\nu$ with respect to $P$ (the $X_{n}$ are a martingale with respect to the $\mathscr{F}_{n}$).
Now, let $P$ be Lebesgue measure on the $\sigma$-field $\mathscr{F}$ of Borel subsets of $\Omega = (0, 1]$, and let $\mathscr{F}_{n}$ be the finite $\sigma$-field generated by the partition of $\Omega$ into dyadic intervals $(k2^{-n},(k+1)2^{-n}],0\leq k \leq 2^{n}$. we know that for every finite measure $\nu$ the Radon-Nikodym derivative is
$$X_{n}(\omega)=\dfrac{\nu(k2^{-n},(k+1)2^{-n}]}{2^{-n}}$$ where $\omega\in(k2^{-n},(k+1)2^{-n}]$. But I don't know how to derive it.
Thanks and Regards!
2026-04-06 18:17:12.1775499432
Radon-Nikodym derivative as a Martingale
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