Potential measures #
The resolvent of a transition family at a shift lam integrates an observable against the
exponentially weighted time average of its transition kernels. This file realises that average
as a genuine measure, the lam-potential measure
laplacePotential lam mu = ∫_0^∞ e^{-lam t} (mu t) dt,
so that both the kernel resolvent of a sub-Markov kernel semigroup and the killed resolvent of an
open set are integrals against a measure on the state space:
SubMarkovKernelSemigroup.lintegral_resolventPotential and
IsConservative.lintegral_killedPotential. Potential measures of sub-Markov families are finite
at every positive shift, with total mass at most 1 / lam.
Two consequences of the measure form are proved here: the killed resolvent is monotone in the
open set and in the observable (IsConservative.killedResolvent_mono), and the kernel resolvent
is measurable in the starting point and continuous along monotone limits of observables
(SubMarkovKernelSemigroup.measurable_kernelResolvent,
SubMarkovKernelSemigroup.kernelResolvent_iSup). The kernel resolvent is also additive and
homogeneous on measurable observables (SubMarkovKernelSemigroup.kernelResolvent_add,
SubMarkovKernelSemigroup.kernelResolvent_const_mul).
No resolvent identity and no topology on the state space are used here.
The exponentially weighted measure on positive times at the shift lam.
Equations
- MarkovProcess.laplaceWeight lam = (MeasureTheory.volume.restrict (Set.Ioi 0)).withDensity fun (t : ℝ) => ENNReal.ofReal (Real.exp (-lam * t))
Instances For
The exponential weight is measurable in time.
At a positive shift the exponentially weighted time measure has total mass 1 / lam.
At a positive shift the exponentially weighted time measure is finite.
The lam-potential measure of a measurable family of transition measures: the exponentially
weighted time average of the family.
Equations
- MarkovProcess.laplacePotential lam mu = (MarkovProcess.laplaceWeight lam).bind mu
Instances For
Integration against a potential measure is the Laplace transform in time of the integrals against the family.
A potential measure of a family of sub-probability measures has mass at most 1 / lam.
A potential measure of a family of sub-probability measures is finite at a positive shift.
The transition measures of a sub-Markov kernel semigroup are measurable in time.
The lam-potential measure of a sub-Markov kernel semigroup started at x.
Equations
- P.resolventPotential lam x = MarkovProcess.laplacePotential lam fun (t : ℝ) => (P.kernel t.toNNReal) x
Instances For
The kernel resolvent is integration against the potential measure.
The potential measure of a sub-Markov kernel semigroup is finite at a positive shift.
At a positive shift the kernel resolvent of the constant observable one is at most
1 / lam.
The normalized potential mass of any set is at most one. At a positive shift the
lam-potential measure of a sub-Markov kernel semigroup has total mass at most 1 / lam, so
the normalization by lam used in the resolvent tail estimates is a sub-probability.
The kernel resolvent is monotone in the observable.
The kernel resolvent is additive on measurable observables.
The kernel resolvent is homogeneous under multiplication by an extended-real constant.
The kernel resolvent is measurable in the starting point.
The kernel resolvent is continuous along monotone limits of observables.
The killed transition kernels are measurable in time.
The lam-potential measure of the process killed at the exit of U, started at x.
Equations
- One or more equations did not get rendered due to their size.
Instances For
The killed resolvent is integration against the killed potential measure.
The killed potential measure is finite at a positive shift.
The killed resolvent is monotone in the open set and in the observable. A path leaves a larger set no earlier, so the killed transition kernels increase with the set.