The integral against a finite signed measure is linear, bounded by the integral of the absolute value against the total variation, defined for bounded measurable functions with bound C times the total variation norm, computable from any splitting of the measure as a difference of finite measures, linear in the measure, equal to the measure on indicators, and equal to the Lebesgue integral when the measure is nonnegative.
In the setting of Radon Measures on Locally Compact Metric Spaces: Standing Notation, let be a measurable space, let and be finite signed measures on , and let . Let and be the total variation and the total variation norm of , and let and be as in Integrable Functions and the Integral with Respect to a Finite Signed Measure (i) and Integrable Functions and the Integral with Respect to a Finite Signed Measure (ii).
Linearity. For and , and
Bound. For , and
Bounded functions. Let be measurable and let with and for every . Then and
Differences of finite measures. Let and be finite measures on with for every , and let be measurable with for every , for some with . Then
Linearity in the measure. Let be measurable with for every , for some with . Then, for the finite signed measures and of Properties of the Total Variation: a Finite Measure, the Jordan Decomposition, Linear Combinations, the Total Variation Norm, and Integrability (v),
Indicators. For every , and
Finite measures. Suppose that for every . Then is a finite measure, the set of Integrable Functions and the Integral with Respect to a Finite Signed Measure (i) is the set of the base, and for every in it the integral of Integrable Functions and the Integral with Respect to a Finite Signed Measure (ii) equals the Lebesgue integral of the base.
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