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Radon-Nikodym Theorem


The Radon-Nikodym theorem asserts that any finite complex measure lambda that is absolutely continuous with respect to a sigma-finite positive measure mu (such as Lebesgue measure on R^n) is given by the integral of some L^1(mu)-function f,

 lambda(E)=int_Efdmu.
(1)

The function f is like a density function for the measure.

A closely related theorem says that any complex measure lambda decomposes into an absolutely continuous measure lambda_a and a singular measure lambda_c. This is the Lebesgue decomposition,

 lambda=lambda_a+lambda_c.
(2)

One consequence of the Radon-Nikodym theorem is that any complex measure has a polar representation

 dmu=hd|mu|,
(3)

with |h|=1.


See also

Absolutely Continuous, Complex Measure, Haar Measure, Lebesgue Decomposition, Lebesgue Measure, Polar Representation, Singular Measure

This entry contributed by Todd Rowland

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References

Hunter, J. K. "Radon-Nikodym Theorem" and "Complex Measures." §6.8 and 6.9 in Measure Theory. 2011. https://www.math.ucdavis.edu/~hunter/measure_theory/measure_notes.pdf.Nagy, G. "Radon-Nikodym Theorems." §4.4 in Real Analysis. pp. 300-321. https://www.math.ksu.edu/~nagy/real-an/.Rudin, W. Real and Complex Analysis. New York: McGraw-Hill, pp. 116-134, 1986.

Referenced on Wolfram|Alpha

Radon-Nikodym Theorem

Cite this as:

Weisstein, Eric W., with contributions by Todd Rowland. "Radon-Nikodym Theorem." From MathWorld--A Wolfram Resource. https://mathworld.wolfram.com/Radon-NikodymTheorem.html

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