For a measurable transformation , a measure is invariant if the pushforward measure equals the original measure, or equivalently for every measurable . This is the measure used in a measure-preserving system.
A multifractal measure has different local scaling behavior at different points. For a measure on a metric space, a basic local exponent, when the limit exists, isIt describes how rapidly mass near shrinks with radius. The Hausdorff dimension of each level set gives a spectrum rather than a single dimension. The word does not require the measure to be invariant, although many examples come from invariant measures of dynamical systems.
For a concrete construction, repeatedly split into halves, giving relative mass to the left half and to the right, with . A level- interval with left choices has length and mass . Along a nested sequence with , its cylinder scaling exponent is . When , different digit frequencies produce different exponents. This is the mechanism by which uneven concentration of mass leads to several scaling laws.
A Borel probability measure is invariant for a Markov kernel semigroup if every transition preserves it. For a Feller semigroup on a compact metric space, it suffices to test the displayed identity on continuous functions. Kernel Jensen inequality gives contraction on , and sup-norm strong continuity followed by density gives strong continuity there for .
For a Feller semigroup on a compact metric space, time-averaged transition laws have weakly convergent subsequences by compactness of probability measures on a compact metric space. Shifting a time interval of length by changes a bounded test-function average by at most . A weak subsequential limit is therefore an invariant probability measure for a semigroup. More generally, tightness of the time averages supplies the required compactness.