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absolutely continuous (Definition)

Let $ \mu$ and $ \nu$ be signed measures on the same measurable space $ (\Omega, \mathscr{S})$. We say that $ \nu$ is absolutely continuous with respect to $ \mu$ if, for each $ A\in \mathscr{S}$ such that $ \vert\mu\vert(A)=0$, it holds that $ \nu(A)=0$. This is usually denoted by $ \nu \ll \mu$.

Remarks.

If $ (\nu^+, \nu^-)$ is the Jordan decomposition of $ \nu$, the following propositions are equivalent:

  1. $ \nu\ll\mu$;
  2. $ \nu^+\ll\mu$ and $ \nu^-\ll\mu$;
  3. $ \vert\nu\vert\ll\vert\mu\vert$.

If $ \nu$ is a finite signed measure and $ \nu\ll\mu$, the following useful property holds: for each $ \varepsilon>0$, there is a $ \delta>0$ such that $ \vert\nu\vert(E)<\varepsilon$ whenever $ \vert\mu\vert(E)<\delta$.



"absolutely continuous" is owned by Koro.
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See Also: Radon-Nikodym theorem, absolutely continuous function

Also defines:  absolute continuity
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Cross-references: property, finite, equivalent, Jordan decomposition, measurable space, signed measures
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This is version 6 of absolutely continuous, born on 2003-02-08, modified 2007-06-28.
Object id is 3997, canonical name is AbsolutelyContinuous.
Accessed 8673 times total.

Classification:
AMS MSC28A12 (Measure and integration :: Classical measure theory :: Contents, measures, outer measures, capacities)

Pending Errata and Addenda
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