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Nu-transform

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In the theory of stochastic processes, a ν-transform is an operation that transforms a measure or a point process into a different point process. Intuitively the ν-transform randomly relocates the points of the point process, with the type of relocation being dependent on the position of each point.

Definition

For measures

Let δ x {\displaystyle \delta _{x}} denote the Dirac measure on the point x {\displaystyle x} and let μ {\displaystyle \mu } be a simple point measure on S {\displaystyle S} . This means that

μ = k δ s k {\displaystyle \mu =\sum _{k}\delta _{s_{k}}}

for distinct s k S {\displaystyle s_{k}\in S} and μ ( B ) < {\displaystyle \mu (B)<\infty } for every bounded set B {\displaystyle B} in S {\displaystyle S} . Further, let ν {\displaystyle \nu } be a Markov kernel from S {\displaystyle S} to T {\displaystyle T} .

Let τ k {\displaystyle \tau _{k}} be independent random elements with distribution ν s k = ν ( s k , ) {\displaystyle \nu _{s_{k}}=\nu (s_{k},\cdot )} . Then the point process

ζ = k δ τ k {\displaystyle \zeta =\sum _{k}\delta _{\tau _{k}}}

is called the ν-transform of the measure μ {\displaystyle \mu } if it is locally finite, meaning that ζ ( B ) < {\displaystyle \zeta (B)<\infty } for every bounded set B {\displaystyle B}

For point processes

For a point process ξ {\displaystyle \xi } , a second point process ζ {\displaystyle \zeta } is called a ν {\displaystyle \nu } -transform of ξ {\displaystyle \xi } if, conditional on { ξ = μ } {\displaystyle \{\xi =\mu \}} , the point process ζ {\displaystyle \zeta } is a ν {\displaystyle \nu } -transform of μ {\displaystyle \mu } .

Properties

Stability

If ζ {\displaystyle \zeta } is a Cox process directed by the random measure ξ {\displaystyle \xi } , then the ν {\displaystyle \nu } -transform of ζ {\displaystyle \zeta } is again a Cox-process, directed by the random measure ξ ν {\displaystyle \xi \cdot \nu } (see Transition kernel#Composition of kernels)

Therefore, the ν {\displaystyle \nu } -transform of a Poisson process with intensity measure μ {\displaystyle \mu } is a Cox process directed by a random measure with distribution μ ν {\displaystyle \mu \cdot \nu } .

Laplace transform

It ζ {\displaystyle \zeta } is a ν {\displaystyle \nu } -transform of ξ {\displaystyle \xi } , then the Laplace transform of ζ {\displaystyle \zeta } is given by

L ζ ( f ) = exp ( log [ exp ( f ( t ) ) μ s ( d t ) ] ξ ( d s ) ) {\displaystyle {\mathcal {L}}_{\zeta }(f)=\exp \left(\int \log \left\xi (\mathrm {d} s)\right)}

for all bounded, positive and measurable functions f {\displaystyle f} .

References

  1. ^ Kallenberg, Olav (2017). Random Measures, Theory and Applications. Switzerland: Springer. p. 73. doi:10.1007/978-3-319-41598-7. ISBN 978-3-319-41596-3.
  2. Kallenberg, Olav (2017). Random Measures, Theory and Applications. Switzerland: Springer. p. 75. doi:10.1007/978-3-319-41598-7. ISBN 978-3-319-41596-3.
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