Markov operator explained

In probability theory and ergodic theory, a Markov operator is an operator on a certain function space that conserves the mass (the so-called Markov property). If the underlying measurable space is topologically sufficiently rich enough, then the Markov operator admits a kernel representation. Markov operators can be linear or non-linear. Closely related to Markov operators is the Markov semigroup.[1]

The definition of Markov operators is not entirely consistent in the literature. Markov operators are named after the Russian mathematician Andrey Markov.

Definitions

Markov operator

Let

(E,l{F})

be a measurable space and

V

a set of real, measurable functions

f:(E,l{F})\to(R,l{B}(R))

.

A linear operator

P

on

V

is a Markov operator if the following is true

P

maps bounded, measurable function on bounded, measurable functions.
  1. Let

1

be the constant function

x\mapsto1

, then

P(1)=1

holds. (conservation of mass / Markov property)
  1. If

f\geq0

then

Pf\geq0

. (conservation of positivity)

Alternative definitions

Some authors define the operators on the Lp spaces as

P:Lp(X)\toLp(Y)

and replace the first condition (bounded, measurable functions on such) with the property[2] [3]

\|Pf\|Y=\|f\|X,\forallf\inLp(X)

Markov semigroup

Let

l{P}=\{Pt\}t\geq

be a family of Markov operators defined on the set of bounded, measurables function on

(E,l{F})

. Then

l{P}

is a Markov semigroup when the following is true

P0=\operatorname{Id}

.

Pt+s=Pt\circPs

for all

t,s\geq0

.

\mu

on

(E,l{F})

that is invariant under

l{P}

, that means for all bounded, positive and measurable functions

f:E\toR

and every

t\geq0

the following holds

\intEPtfd\mu=\intEfd\mu

.

Dual semigroup

Each Markov semigroup

l{P}=\{Pt\}t\geq

induces a dual semigroup
*
(P
t)

t\geq

through

\intEPtfd\mu=\intE

*
fd\left(P
t\mu\right).
If

\mu

is invariant under

l{P}

then
*
P
t\mu=\mu
.

Infinitesimal generator of the semigroup

Let

\{Pt\}t\geq

be a family of bounded, linear Markov operators on the Hilbert space

L2(\mu)

, where

\mu

is an invariant measure. The infinitesimal generator

L

of the Markov semigroup

l{P}=\{Pt\}t\geq

is defined as

Lf=\lim\limitst\downarrow

Ptf-f
t

,

and the domain

D(L)

is the

L2(\mu)

-space of all such functions where this limit exists and is in

L2(\mu)

again.[4]

D(L)=\left\{f\inL2(\mu):\lim\limitst\downarrow

Ptf-f
t

existsandisinL2(\mu)\right\}.

\Gamma

measuers how far

L

is from being a derivation.

Kernel representation of a Markov operator

A Markov operator

Pt

has a kernel representation

(Ptf)(x)=\intEf(y)pt(x,dy),x\inE,

with respect to some probability kernel

pt(x,A)

, if the underlying measurable space

(E,l{F})

has the following sufficient topological properties:

\mu:l{F} x l{F}\to[0,1]

can be decomposed as

\mu(dx,dy)=k(x,dy)\mu1(dx)

, where

\mu1

is the projection onto the first component and

k(x,dy)

is a probability kernel.

l{F}

.If one defines now a σ-finite measure on

(E,l{F})

then it is possible to prove that ever Markov operator

P

admits such a kernel representation with respect to

k(x,dy)

.

Literature

References

  1. Book: Analysis and Geometry of Markov Diffusion Operators. Dominique. Bakry. Ivan. Gentil. Michel. Ledoux. Springer Cham. 10.1007/978-3-319-00227-9.
  2. Book: Tanja. Eisner. Bálint. Farkas. Markus. Haase. Rainer. Nagel. 2015. Operator Theoretic Aspects of Ergodic Theory. Markov Operators. Graduate Texts in Mathematics. 2727. Springer. Cham. 10.1007/978-3-319-16898-2. 249.
  3. Book: Wang, Fengyu. Functional Inequalities Markov Semigroups and Spectral Theory. Ukraine. Elsevier Science. 2006. 3.
  4. Book: Wang, Fengyu. Functional Inequalities Markov Semigroups and Spectral Theory. Ukraine. Elsevier Science. 2006. 1.