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Chapter 3 - Poisson process
Chapter 3 - Poisson process
Nial Friel Stochastic Models - STAT30090 - STAT40680
Chapter 3 - Poisson processDefinition of a Poisson processMain propertiesSome extensions
Counting processes
Counting processes are increasing processes {Xt , t ∈ R+} withXt ∈ N.
NotationThe idea is to count something over time (eg, the arrivals ofcustomers, ...) : Xt is the number of arrivals between time 0and time t so naturally we set X0 = 0.Let N(s,t] be the number of arrivals during the interval (s, t] :
N(s,t] = Xt − Xs .
Note that Xt = N(0,t].
Nial Friel Stochastic Models - STAT30090 - STAT40680
Chapter 3 - Poisson processDefinition of a Poisson processMain propertiesSome extensions
Counting processes
Counting processes are increasing processes {Xt , t ∈ R+} withXt ∈ N.
NotationThe idea is to count something over time (eg, the arrivals ofcustomers, ...) : Xt is the number of arrivals between time 0and time t so naturally we set X0 = 0.
Let N(s,t] be the number of arrivals during the interval (s, t] :
N(s,t] = Xt − Xs .
Note that Xt = N(0,t].
Nial Friel Stochastic Models - STAT30090 - STAT40680
Chapter 3 - Poisson processDefinition of a Poisson processMain propertiesSome extensions
Counting processes
Counting processes are increasing processes {Xt , t ∈ R+} withXt ∈ N.
NotationThe idea is to count something over time (eg, the arrivals ofcustomers, ...) : Xt is the number of arrivals between time 0and time t so naturally we set X0 = 0.Let N(s,t] be the number of arrivals during the interval (s, t] :
N(s,t] = Xt − Xs .
Note that Xt = N(0,t].
Nial Friel Stochastic Models - STAT30090 - STAT40680
Chapter 3 - Poisson processDefinition of a Poisson processMain propertiesSome extensions
Definition of a Poisson process
Poisson processA Poisson process with intensity λ > 0 is a counting process{Xt} with
1 independent increments ;2 P(Xt+h − Xt = 1) = λh + o(h) when h→ 0 ;3 P(Xt+h − Xt > 1) = o(h) when h→ 0.
Nial Friel Stochastic Models - STAT30090 - STAT40680
Chapter 3 - Poisson processDefinition of a Poisson processMain propertiesSome extensions
Some remarks about (1)
Recall that by “independent increments” we mean that, for anyt1 < t1 ≤ t3 < t4,
Xt2 − Xt1 indep. of Xt4 − Xt3 .
In other words :
N(t1,t2] is indep. of N(t3,t4].
This is sometimes referred as the loss of memory property.
Nial Friel Stochastic Models - STAT30090 - STAT40680
Chapter 3 - Poisson processDefinition of a Poisson processMain propertiesSome extensions
Some remarks about (1)
Recall that by “independent increments” we mean that, for anyt1 < t1 ≤ t3 < t4,
Xt2 − Xt1 indep. of Xt4 − Xt3 .
In other words :
N(t1,t2] is indep. of N(t3,t4].
This is sometimes referred as the loss of memory property.
Nial Friel Stochastic Models - STAT30090 - STAT40680
Chapter 3 - Poisson processDefinition of a Poisson processMain propertiesSome extensions
Some remarks about (1)
Recall that by “independent increments” we mean that, for anyt1 < t1 ≤ t3 < t4,
Xt2 − Xt1 indep. of Xt4 − Xt3 .
In other words :
N(t1,t2] is indep. of N(t3,t4].
This is sometimes referred as the loss of memory property.
Nial Friel Stochastic Models - STAT30090 - STAT40680
Chapter 3 - Poisson processDefinition of a Poisson processMain propertiesSome extensions
Remarks on (2) and (3)Recall (2) and (3) :
P(Xt+h − Xt = 1) = λh + o(h),
P(Xt+h − Xt > 1) = o(h).
We can write (3) in a different way :
P(Xt+h − Xt > 1)
h−−→h→0
0.
Two customers will never arrive exactly at the same time, andthe probability that two customers arrive at a very small periodof time is negligible. Remark that (2) and (3) imply that :
P(Xt+h − Xt = 0) = 1− λh + o(h).
Nial Friel Stochastic Models - STAT30090 - STAT40680
Chapter 3 - Poisson processDefinition of a Poisson processMain propertiesSome extensions
Remarks on (2) and (3)Recall (2) and (3) :
P(Xt+h − Xt = 1) = λh + o(h),
P(Xt+h − Xt > 1) = o(h).
We can write (3) in a different way :
P(Xt+h − Xt > 1)
h−−→h→0
0.
Two customers will never arrive exactly at the same time, andthe probability that two customers arrive at a very small periodof time is negligible. Remark that (2) and (3) imply that :
P(Xt+h − Xt = 0) = 1− λh + o(h).
Nial Friel Stochastic Models - STAT30090 - STAT40680
Chapter 3 - Poisson processDefinition of a Poisson processMain propertiesSome extensions
Remarks on (2) and (3)Recall (2) and (3) :
P(Xt+h − Xt = 1) = λh + o(h),
P(Xt+h − Xt > 1) = o(h).
We can write (3) in a different way :
P(Xt+h − Xt > 1)
h−−→h→0
0.
Two customers will never arrive exactly at the same time, andthe probability that two customers arrive at a very small periodof time is negligible.
Remark that (2) and (3) imply that :
P(Xt+h − Xt = 0) = 1− λh + o(h).
Nial Friel Stochastic Models - STAT30090 - STAT40680
Chapter 3 - Poisson processDefinition of a Poisson processMain propertiesSome extensions
Remarks on (2) and (3)Recall (2) and (3) :
P(Xt+h − Xt = 1) = λh + o(h),
P(Xt+h − Xt > 1) = o(h).
We can write (3) in a different way :
P(Xt+h − Xt > 1)
h−−→h→0
0.
Two customers will never arrive exactly at the same time, andthe probability that two customers arrive at a very small periodof time is negligible. Remark that (2) and (3) imply that :
P(Xt+h − Xt = 0) = 1− λh + o(h).
Nial Friel Stochastic Models - STAT30090 - STAT40680
Chapter 3 - Poisson processDefinition of a Poisson processMain propertiesSome extensions
About Poisson
Siméon Denis Poisson (1781-1840), the French mathematicianand physicist, who received the Copley medal from the RoyalSociety of London in 1832.
Nial Friel Stochastic Models - STAT30090 - STAT40680
Chapter 3 - Poisson processDefinition of a Poisson processMain propertiesSome extensions
Fundamental theorem
A reminder : the Poisson distribution
U ∼ P(`)⇔ for any k ∈ N, P(U = k) =`k
k!e−`.
Then :E(U) = Var(U) = `.U ∼ P(`)⇔ for any s > 0, E
(esU)
= eλ(es−1).
TheoremLet {Xt} be a Poisson process with intensity λ andN(s,t] = Xt − Xs for s < t. Then
N(s,t] ∼ P(λ(t − s)).
Nial Friel Stochastic Models - STAT30090 - STAT40680
Chapter 3 - Poisson processDefinition of a Poisson processMain propertiesSome extensions
Fundamental theorem
A reminder : the Poisson distribution
U ∼ P(`)⇔ for any k ∈ N, P(U = k) =`k
k!e−`.
Then :E(U) = Var(U) = `.U ∼ P(`)⇔ for any s > 0, E
(esU)
= eλ(es−1).
TheoremLet {Xt} be a Poisson process with intensity λ andN(s,t] = Xt − Xs for s < t. Then
N(s,t] ∼ P(λ(t − s)).
Nial Friel Stochastic Models - STAT30090 - STAT40680
Chapter 3 - Poisson processDefinition of a Poisson processMain propertiesSome extensions
An immediate consequence
The arrival rateThe arrival rate between times s and t is :
Xt − Xs
t − s.
Consequence of the theoremFor a Poisson process, the expected arrival rate is constant,equal to λ :
E[Xt − Xs
t − s
]= λ.
Nial Friel Stochastic Models - STAT30090 - STAT40680
Chapter 3 - Poisson processDefinition of a Poisson processMain propertiesSome extensions
An immediate consequence
The arrival rateThe arrival rate between times s and t is :
Xt − Xs
t − s.
Consequence of the theoremFor a Poisson process, the expected arrival rate is constant,equal to λ :
E[Xt − Xs
t − s
]= λ.
Nial Friel Stochastic Models - STAT30090 - STAT40680
Chapter 3 - Poisson processDefinition of a Poisson processMain propertiesSome extensions
Arrival times
DefinitionLet S1, S2, ... be the arrival times :
Sk = inf{t ≥ 0 : Xt = k}
(and by convention S0 = 0).
Note that :
Xt =∞∑i=1
1Si≤t .
Nial Friel Stochastic Models - STAT30090 - STAT40680
Chapter 3 - Poisson processDefinition of a Poisson processMain propertiesSome extensions
Arrival times
DefinitionLet S1, S2, ... be the arrival times :
Sk = inf{t ≥ 0 : Xt = k}
(and by convention S0 = 0).
Note that :
Xt =∞∑i=1
1Si≤t .
Nial Friel Stochastic Models - STAT30090 - STAT40680
Chapter 3 - Poisson processDefinition of a Poisson processMain propertiesSome extensions
Distribution of the arrival times
TheoremFor any k ≥ 1, Sk ∼ Γ(k , λ) where we recall that the Γ(k , λ)distribution has density :
f (x) =λk
Γ(k)e−λxxk−1.
Nial Friel Stochastic Models - STAT30090 - STAT40680
Chapter 3 - Poisson processDefinition of a Poisson processMain propertiesSome extensions
Gap between arrival times
DefinitionFor any k ≥ 1, Tk = Sk − Sk−1.
TheoremThe Tk are iid with distribution E(λ), where we recall that theexponential distribution E(λ) has density
f (x) = λe−λx .
In particular, E(Tk) = 1/λ and Var(Tk) = 1/λ2.
Nial Friel Stochastic Models - STAT30090 - STAT40680
Chapter 3 - Poisson processDefinition of a Poisson processMain propertiesSome extensions
Gap between arrival times
DefinitionFor any k ≥ 1, Tk = Sk − Sk−1.
TheoremThe Tk are iid with distribution E(λ), where we recall that theexponential distribution E(λ) has density
f (x) = λe−λx .
In particular, E(Tk) = 1/λ and Var(Tk) = 1/λ2.
Nial Friel Stochastic Models - STAT30090 - STAT40680
Chapter 3 - Poisson processDefinition of a Poisson processMain propertiesSome extensions
Subdividing an interval with a given count
Question : suppose we know that Xt = n. How are the arrivaltimes S1, S2, ..., Sn distributed within the interval [0, t] ?
Example : Xt = 1. Then for 0 < s < t,
P (S1 < s|Xt = 1) =P (S1 < s,Xt = 1)
P (Xt = 1)
=P(N(0,s] = 1,N(s,t] = 0
)P(N(0,t] = 1
)=λse−λse−λ(t−s)
λte−λt =st
in other words, L(S1|Xt = 1) = U [0, t] the uniformdistribution on [0, t].
Nial Friel Stochastic Models - STAT30090 - STAT40680
Chapter 3 - Poisson processDefinition of a Poisson processMain propertiesSome extensions
Subdividing an interval with a given count
Question : suppose we know that Xt = n. How are the arrivaltimes S1, S2, ..., Sn distributed within the interval [0, t] ?Example : Xt = 1. Then for 0 < s < t,
P (S1 < s|Xt = 1) =P (S1 < s,Xt = 1)
P (Xt = 1)
=P(N(0,s] = 1,N(s,t] = 0
)P(N(0,t] = 1
)=λse−λse−λ(t−s)
λte−λt =st
in other words, L(S1|Xt = 1) = U [0, t] the uniformdistribution on [0, t].
Nial Friel Stochastic Models - STAT30090 - STAT40680
Chapter 3 - Poisson processDefinition of a Poisson processMain propertiesSome extensions
Subdividing an interval with a given count
Question : suppose we know that Xt = n. How are the arrivaltimes S1, S2, ..., Sn distributed within the interval [0, t] ?Example : Xt = 1. Then for 0 < s < t,
P (S1 < s|Xt = 1) =P (S1 < s,Xt = 1)
P (Xt = 1)
=P(N(0,s] = 1,N(s,t] = 0
)P(N(0,t] = 1
)=λse−λse−λ(t−s)
λte−λt =st
in other words, L(S1|Xt = 1) = U [0, t] the uniformdistribution on [0, t].
Nial Friel Stochastic Models - STAT30090 - STAT40680
Chapter 3 - Poisson processDefinition of a Poisson processMain propertiesSome extensions
Subdividing an interval with a given count
TheoremLet U1, U2, ..., Un be an iid sample with a uniform distributionU [0, t]. Let U(1), ..., U(n) be the corresponding order statistic,ie :{U1, . . . ,Un} = {U(1), . . . ,U(n)} ;U(1) ≤ · · · ≤ U(n).
Then L(S1, . . . , Sn|Xt = n) = L(U(1), . . . ,U(n)).
In other words, conditional on Xt = n, the n arrivals areuniformly distributed on [0, t].
Nial Friel Stochastic Models - STAT30090 - STAT40680
Chapter 3 - Poisson processDefinition of a Poisson processMain propertiesSome extensions
Subdividing an interval with a given count
TheoremLet U1, U2, ..., Un be an iid sample with a uniform distributionU [0, t]. Let U(1), ..., U(n) be the corresponding order statistic,ie :{U1, . . . ,Un} = {U(1), . . . ,U(n)} ;U(1) ≤ · · · ≤ U(n).
Then L(S1, . . . , Sn|Xt = n) = L(U(1), . . . ,U(n)).
In other words, conditional on Xt = n, the n arrivals areuniformly distributed on [0, t].
Nial Friel Stochastic Models - STAT30090 - STAT40680
Chapter 3 - Poisson processDefinition of a Poisson processMain propertiesSome extensions
Marked Poisson process
Defintion - marked Poisson processA marked Poisson process is defined as :
a Poisson process {Xt , t ≥ 0} with arrival times S1, S2, ...a collection of iid random variables M1, M2, ... indep. of{Xt}.
For example :Sk is the arrival time of the k-th customer.Mk is the money spent by the k-th customer.
Or :Sk is the time of occurence of the k-th earthquake ;Mk is its magnitude.
...
Nial Friel Stochastic Models - STAT30090 - STAT40680
Chapter 3 - Poisson processDefinition of a Poisson processMain propertiesSome extensions
Marked Poisson process
Defintion - marked Poisson processA marked Poisson process is defined as :
a Poisson process {Xt , t ≥ 0} with arrival times S1, S2, ...a collection of iid random variables M1, M2, ... indep. of{Xt}.
For example :Sk is the arrival time of the k-th customer.Mk is the money spent by the k-th customer.
Or :Sk is the time of occurence of the k-th earthquake ;Mk is its magnitude.
...
Nial Friel Stochastic Models - STAT30090 - STAT40680
Chapter 3 - Poisson processDefinition of a Poisson processMain propertiesSome extensions
Marked Poisson process
Defintion - marked Poisson processA marked Poisson process is defined as :
a Poisson process {Xt , t ≥ 0} with arrival times S1, S2, ...a collection of iid random variables M1, M2, ... indep. of{Xt}.
For example :Sk is the arrival time of the k-th customer.Mk is the money spent by the k-th customer.
Or :Sk is the time of occurence of the k-th earthquake ;Mk is its magnitude.
...Nial Friel Stochastic Models - STAT30090 - STAT40680
Chapter 3 - Poisson processDefinition of a Poisson processMain propertiesSome extensions
Thinned Poisson process
Definition - thinned Poisson processLet {Xt} be a marked Poisson process with arrival times S1,S2, ... and marks M1, M2, ... ∼ Be(p). We define the thinnedPoisson process {Yt} by
Yt =∞∑i=1
1Si≤t,Mi=1.
In other words, {Yt} is obtained from {Xt} by erasing thearrivals Si with Mi = 0.
TheoremThe process {Yt} is actually a Poisson process with parameterpλ.
Nial Friel Stochastic Models - STAT30090 - STAT40680
Chapter 3 - Poisson processDefinition of a Poisson processMain propertiesSome extensions
Thinned Poisson process
Definition - thinned Poisson processLet {Xt} be a marked Poisson process with arrival times S1,S2, ... and marks M1, M2, ... ∼ Be(p). We define the thinnedPoisson process {Yt} by
Yt =∞∑i=1
1Si≤t,Mi=1.
In other words, {Yt} is obtained from {Xt} by erasing thearrivals Si with Mi = 0.
TheoremThe process {Yt} is actually a Poisson process with parameterpλ.
Nial Friel Stochastic Models - STAT30090 - STAT40680
Chapter 3 - Poisson processDefinition of a Poisson processMain propertiesSome extensions
Superposition of Poisson process
TheoremLet {Xt} and {Yt} be two Poisson processes independent ofeach other, with intensity given by λ and µ, respectively. Letus put Zt = Xt + Yt .
Then {Zt} is a Poisson process withintensity λ + µ.
Nial Friel Stochastic Models - STAT30090 - STAT40680
Chapter 3 - Poisson processDefinition of a Poisson processMain propertiesSome extensions
Superposition of Poisson process
TheoremLet {Xt} and {Yt} be two Poisson processes independent ofeach other, with intensity given by λ and µ, respectively. Letus put Zt = Xt + Yt . Then {Zt} is a Poisson process withintensity λ + µ.
Nial Friel Stochastic Models - STAT30090 - STAT40680
Chapter 3 - Poisson processDefinition of a Poisson processMain propertiesSome extensions
Campbell’s Theorem
Campbell’s TheoremFor a Poisson process {Xt} with arrival times S1, S2, ... andfor any function f integrable on [0, t], we have
E
[Xt∑i=1
f (Si)
]= λ
∫ t
0f (s)ds.
Nial Friel Stochastic Models - STAT30090 - STAT40680
Chapter 3 - Poisson processDefinition of a Poisson processMain propertiesSome extensions
Campbell’s Theorem for marked processes
Campbell’s Theorem for marked processesFor a marked Poisson process {Xt} with arrival times S1, S2,..., marks M1, M2, ... ∈M and for any function f integrableon [0, t]×M, we have
E
[Xt∑i=1
f (Si ,Mi)
]= λ
∫ t
0E [f (s,M1)] ds.
Nial Friel Stochastic Models - STAT30090 - STAT40680
Chapter 3 - Poisson processDefinition of a Poisson processMain propertiesSome extensions
Application of Campbell’s TheoremA squirrel drinks in a river at random times given by a Poissonprocess : S1, S2...
Unfortunately, the river is contaminated by adangerous substance, and at each time he absorbs a randomquantity Mi of poison. Each dose of poison is eliminated by hisbody at an exponential rate.In other words, the quantity of poison in his body at time t is :
Q =Xt∑i=1
Mie−α(t−Si ).
Thanks to Campbell’s Theorem one can compute
E(Q) = λ
∫ t
0E(Mie−α(t−s))ds =
λE(M1)
α
(1− e−αt) .
Nial Friel Stochastic Models - STAT30090 - STAT40680
Chapter 3 - Poisson processDefinition of a Poisson processMain propertiesSome extensions
Application of Campbell’s TheoremA squirrel drinks in a river at random times given by a Poissonprocess : S1, S2... Unfortunately, the river is contaminated by adangerous substance, and at each time he absorbs a randomquantity Mi of poison.
Each dose of poison is eliminated by hisbody at an exponential rate.In other words, the quantity of poison in his body at time t is :
Q =Xt∑i=1
Mie−α(t−Si ).
Thanks to Campbell’s Theorem one can compute
E(Q) = λ
∫ t
0E(Mie−α(t−s))ds =
λE(M1)
α
(1− e−αt) .
Nial Friel Stochastic Models - STAT30090 - STAT40680
Chapter 3 - Poisson processDefinition of a Poisson processMain propertiesSome extensions
Application of Campbell’s TheoremA squirrel drinks in a river at random times given by a Poissonprocess : S1, S2... Unfortunately, the river is contaminated by adangerous substance, and at each time he absorbs a randomquantity Mi of poison. Each dose of poison is eliminated by hisbody at an exponential rate.
In other words, the quantity of poison in his body at time t is :
Q =Xt∑i=1
Mie−α(t−Si ).
Thanks to Campbell’s Theorem one can compute
E(Q) = λ
∫ t
0E(Mie−α(t−s))ds =
λE(M1)
α
(1− e−αt) .
Nial Friel Stochastic Models - STAT30090 - STAT40680
Chapter 3 - Poisson processDefinition of a Poisson processMain propertiesSome extensions
Application of Campbell’s TheoremA squirrel drinks in a river at random times given by a Poissonprocess : S1, S2... Unfortunately, the river is contaminated by adangerous substance, and at each time he absorbs a randomquantity Mi of poison. Each dose of poison is eliminated by hisbody at an exponential rate.In other words, the quantity of poison in his body at time t is :
Q =Xt∑i=1
Mie−α(t−Si ).
Thanks to Campbell’s Theorem one can compute
E(Q) = λ
∫ t
0E(Mie−α(t−s))ds =
λE(M1)
α
(1− e−αt) .
Nial Friel Stochastic Models - STAT30090 - STAT40680
Chapter 3 - Poisson processDefinition of a Poisson processMain propertiesSome extensions
Application of Campbell’s TheoremA squirrel drinks in a river at random times given by a Poissonprocess : S1, S2... Unfortunately, the river is contaminated by adangerous substance, and at each time he absorbs a randomquantity Mi of poison. Each dose of poison is eliminated by hisbody at an exponential rate.In other words, the quantity of poison in his body at time t is :
Q =Xt∑i=1
Mie−α(t−Si ).
Thanks to Campbell’s Theorem one can compute
E(Q) = λ
∫ t
0E(Mie−α(t−s))ds =
λE(M1)
α
(1− e−αt) .
Nial Friel Stochastic Models - STAT30090 - STAT40680
Chapter 3 - Poisson processDefinition of a Poisson processMain propertiesSome extensions
Inhomogeneous Poisson process : definition
In some cases, the assumption that the expected arrival rate isconstant is not realistic. For example, customers are morelikely to come to a shop after 5pm than before.
DefinitionLet λ(t) > 0 be a function of the time t. An inhomogeneousPoisson process with intensity λ(t) is a counting process {Xt}with
1 independent increments ;2 P(Xt+h − Xt = 1) = λ(t)h + o(h) when h→ 0 ;3 P(Xt+h − Xt > 1) = o(h) when h→ 0.
Nial Friel Stochastic Models - STAT30090 - STAT40680
Chapter 3 - Poisson processDefinition of a Poisson processMain propertiesSome extensions
Inhomogeneous Poisson process : definition
In some cases, the assumption that the expected arrival rate isconstant is not realistic. For example, customers are morelikely to come to a shop after 5pm than before.
DefinitionLet λ(t) > 0 be a function of the time t. An inhomogeneousPoisson process with intensity λ(t) is a counting process {Xt}with
1 independent increments ;2 P(Xt+h − Xt = 1) = λ(t)h + o(h) when h→ 0 ;3 P(Xt+h − Xt > 1) = o(h) when h→ 0.
Nial Friel Stochastic Models - STAT30090 - STAT40680
Chapter 3 - Poisson processDefinition of a Poisson processMain propertiesSome extensions
Inhomogeneous Poisson process : properties
Let {Xt} be an inhomogeneous Poisson process with intensityλ(t). Then we can prove that
N(s,t] = Xt − Xs ∼ P(∫ t
sλ(x)dx
).
In particular, when λ(t) = λ is constant, {Xt} is a Poissonprocess and we have :
N(s,t] = Xt − Xs ∼ P ((t − s)λ) .
Nial Friel Stochastic Models - STAT30090 - STAT40680
Chapter 3 - Poisson processDefinition of a Poisson processMain propertiesSome extensions
Inhomogeneous Poisson process : properties
Let {Xt} be an inhomogeneous Poisson process with intensityλ(t). Then we can prove that
N(s,t] = Xt − Xs ∼ P(∫ t
sλ(x)dx
).
In particular, when λ(t) = λ is constant, {Xt} is a Poissonprocess and we have :
N(s,t] = Xt − Xs ∼ P ((t − s)λ) .
Nial Friel Stochastic Models - STAT30090 - STAT40680
Chapter 3 - Poisson processDefinition of a Poisson processMain propertiesSome extensions
Planar Poisson point process
It is also possible to extend the Poisson process to the casewhere the index t does not belong to R but to R2. In this case,t does not refer to the time but to a position in the plane.
It is more convenient to extend the definition of the arrivaltimes S1, S2, ...A Poisson process on the plane is a random family of points Ssuch that
the number of each point in the region K is distributedaccording to P(λ.area(K )) ;inside a region K , the points are uniformly distributed ;the number of points in two disjoints regions K1 and K2 isindependent.
Nial Friel Stochastic Models - STAT30090 - STAT40680
Chapter 3 - Poisson processDefinition of a Poisson processMain propertiesSome extensions
Planar Poisson point process
It is also possible to extend the Poisson process to the casewhere the index t does not belong to R but to R2. In this case,t does not refer to the time but to a position in the plane.It is more convenient to extend the definition of the arrivaltimes S1, S2, ...
A Poisson process on the plane is a random family of points Ssuch that
the number of each point in the region K is distributedaccording to P(λ.area(K )) ;inside a region K , the points are uniformly distributed ;the number of points in two disjoints regions K1 and K2 isindependent.
Nial Friel Stochastic Models - STAT30090 - STAT40680
Chapter 3 - Poisson processDefinition of a Poisson processMain propertiesSome extensions
Planar Poisson point process
It is also possible to extend the Poisson process to the casewhere the index t does not belong to R but to R2. In this case,t does not refer to the time but to a position in the plane.It is more convenient to extend the definition of the arrivaltimes S1, S2, ...A Poisson process on the plane is a random family of points Ssuch that
the number of each point in the region K is distributedaccording to P(λ.area(K )) ;inside a region K , the points are uniformly distributed ;the number of points in two disjoints regions K1 and K2 isindependent.
Nial Friel Stochastic Models - STAT30090 - STAT40680