residuals and goodness-of-fit tests for marked gibbs point...
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Residuals and Goodness-of-fit tests for marked Gibbspoint processes
Frederic Lavancier(Laboratoire de Mathematiques Jean Leray, Nantes, France)
Joint work with J.-F. Coeurjolly (Grenoble, France)
27/06/2012
F. Lavancier () Residuals and GoF tests for Gibbs pp 27/06/2012 1 / 19
1 Gibbs point processes
2 Validations through residualsResiduals for spatial point processesAsymptoticsMeasures of departures to the true model
F. Lavancier () Residuals and GoF tests for Gibbs pp 27/06/2012 2 / 19
Type of data
Question :−→ Independence or interaction between locations and/or between marks ?
F. Lavancier () Residuals and GoF tests for Gibbs pp 27/06/2012 3 / 19
Type of data
Question :−→ Independence or interaction between locations and/or between marks ?
F. Lavancier () Residuals and GoF tests for Gibbs pp 27/06/2012 3 / 19
Marked point processes
State space : S := Rd ×M associated to the measure µ = λ⊗ λm.
I λ denotes the Lebesgue measure on Rd .I M is a measurable space, endowed with the probability measure λm.
Rd is the space of points and M the space of marks.
Let denote xm = (x ,m) an element of Rd ×M, i.e. a marked point.
ϕ denotes a locally finite point configuration in S.
ϕΛ is the restriction of ϕ on Λ : ϕΛ = ϕ ∩ Λ.
Ω is the space of locally finite point configurations ϕ.
Definition (marked point process)
A marked point process is a random variable on Ω.
Example :
π : the standard (non-marked) Poisson point process.
F. Lavancier () Residuals and GoF tests for Gibbs pp 27/06/2012 4 / 19
Marked point processes
State space : S := Rd ×M associated to the measure µ = λ⊗ λm.
I λ denotes the Lebesgue measure on Rd .I M is a measurable space, endowed with the probability measure λm.
Rd is the space of points and M the space of marks.
Let denote xm = (x ,m) an element of Rd ×M, i.e. a marked point.
ϕ denotes a locally finite point configuration in S.
ϕΛ is the restriction of ϕ on Λ : ϕΛ = ϕ ∩ Λ.
Ω is the space of locally finite point configurations ϕ.
Definition (marked point process)
A marked point process is a random variable on Ω.
Example :
π : the standard (non-marked) Poisson point process.
F. Lavancier () Residuals and GoF tests for Gibbs pp 27/06/2012 4 / 19
Marked point processes
State space : S := Rd ×M associated to the measure µ = λ⊗ λm.
I λ denotes the Lebesgue measure on Rd .I M is a measurable space, endowed with the probability measure λm.
Rd is the space of points and M the space of marks.
Let denote xm = (x ,m) an element of Rd ×M, i.e. a marked point.
ϕ denotes a locally finite point configuration in S.
ϕΛ is the restriction of ϕ on Λ : ϕΛ = ϕ ∩ Λ.
Ω is the space of locally finite point configurations ϕ.
Definition (marked point process)
A marked point process is a random variable on Ω.
Example :
π : the standard (non-marked) Poisson point process.
F. Lavancier () Residuals and GoF tests for Gibbs pp 27/06/2012 4 / 19
Marked point processes
State space : S := Rd ×M associated to the measure µ = λ⊗ λm.
I λ denotes the Lebesgue measure on Rd .I M is a measurable space, endowed with the probability measure λm.
Rd is the space of points and M the space of marks.
Let denote xm = (x ,m) an element of Rd ×M, i.e. a marked point.
ϕ denotes a locally finite point configuration in S.
ϕΛ is the restriction of ϕ on Λ : ϕΛ = ϕ ∩ Λ.
Ω is the space of locally finite point configurations ϕ.
Definition (marked point process)
A marked point process is a random variable on Ω.
Example :
π : the standard (non-marked) Poisson point process.
F. Lavancier () Residuals and GoF tests for Gibbs pp 27/06/2012 4 / 19
Marked point processes
State space : S := Rd ×M associated to the measure µ = λ⊗ λm.
I λ denotes the Lebesgue measure on Rd .I M is a measurable space, endowed with the probability measure λm.
Rd is the space of points and M the space of marks.
Let denote xm = (x ,m) an element of Rd ×M, i.e. a marked point.
ϕ denotes a locally finite point configuration in S.
ϕΛ is the restriction of ϕ on Λ : ϕΛ = ϕ ∩ Λ.
Ω is the space of locally finite point configurations ϕ.
Definition (marked point process)
A marked point process is a random variable on Ω.
Example :
π : the standard (non-marked) Poisson point process.
F. Lavancier () Residuals and GoF tests for Gibbs pp 27/06/2012 4 / 19
Gibbs measures
Let (VΛ)Λ∈B(Rd ) be a family of energies (or Hamiltonian)
VΛ : Ω −→ R ∪ +∞ϕ 7−→ VΛ(ϕΛ|ϕΛc )
VΛ(ϕ) is the energy of ϕΛ inside Λ given the outside configuration ϕΛc
Definition
A probability measure P on Ω is a Gibbs measure associated to the family(VΛ)Λ if for every bounded set Λ and P-almost every ϕΛc
P(dϕΛ|ϕΛc ) ∝ e−VΛ(ϕΛ|ϕΛc ) πΛ(dϕΛ).
F. Lavancier () Residuals and GoF tests for Gibbs pp 27/06/2012 5 / 19
Example : Strauss marked point process, M = r , b
VΛ(ϕ; θ) = θ11|ϕrΛ|+ θ12|ϕb
Λ|
+ θ21
∑(x r ,y r )
1||y r−x r ||<10 + θ22
∑(xb,yb)
1||yb−xb||<10 + θ23
∑(xb,y r )
1||y r−xb||<10
F. Lavancier () Residuals and GoF tests for Gibbs pp 27/06/2012 6 / 19
Gibbs Voronoi tessellation
VΛ(ϕ) =∑
C∈ Vor(ϕ)C∩Λ 6=∅
V1(C ) +∑
C ,C ′∈ Vor(ϕ)C and C ′are neighbors
(C∪C ′)∩Λ 6=∅
V2(C ,C ′)
V1(C ) : deals with the shape of the cell and V2(C ,C ′) = θ |vol(C )− vol(C ′)|.
θ > 0 θ < 0
F. Lavancier () Residuals and GoF tests for Gibbs pp 27/06/2012 7 / 19
1 Gibbs point processes
2 Validations through residualsResiduals for spatial point processesAsymptoticsMeasures of departures to the true model
F. Lavancier () Residuals and GoF tests for Gibbs pp 27/06/2012 8 / 19
Motivation
In pratice, for a given data set :
1 Propose one reasonable model, i.e. choose (VΛ(.; θ))Λ∈B(R[d]).
2 Estimate θ? (different methods are available)
3 Assess the adequation of the fitted model to the data ⇒ Residuals.
For Gibbs point processes :
1 How to define residuals ?
2 Theoretical properties of residuals ?
3 Construction of Goodness-of-fits tests.
F. Lavancier () Residuals and GoF tests for Gibbs pp 27/06/2012 9 / 19
Motivation
In pratice, for a given data set :
1 Propose one reasonable model, i.e. choose (VΛ(.; θ))Λ∈B(R[d]).
2 Estimate θ? (different methods are available)
3 Assess the adequation of the fitted model to the data ⇒ Residuals.
For Gibbs point processes :
1 How to define residuals ?
2 Theoretical properties of residuals ?
3 Construction of Goodness-of-fits tests.
F. Lavancier () Residuals and GoF tests for Gibbs pp 27/06/2012 9 / 19
The h-residuals Baddeley, Turner, Møller, Hazelton (05)
h−innovations (in Λ) : for any function h(·, ·; θ) : S× Ω→ R,
IΛ(ϕ; h, θ?) :=∑
xm∈ϕΛ
h(xm, ϕ \ xm; θ?)−∫
Λ×Mh(xm, ϕ; θ?)e−V (xm|ϕ;θ?)µ(dxm)
where V (xm|ϕ; θ) := VΛ(ϕ ∪ xm; θ)− VΛ(ϕ; θ) is the local energy of xm in ϕ.
h−residuals (in Λ) : RΛ(ϕ; h, θ) := IΛ(ϕ; h, θ)
Theoretical Motivation :
Theorem (Georgii-Nguyen-Zessin)
For any h(·, ·; θ) : S× Ω→ R, for any θ ∈ Θ,
Eθ?
(∑xm∈ϕ
h (xm, ϕ \ xm; θ)
)= Eθ?
(∫Rd×M
h (xm, ϕ; θ) e−V (xm|ϕ;θ?)µ(dxm)
)
Conjecture from BTMH : RΛ(ϕ; h, θ) ≈ 0 and |Λ|1/2RΛ(ϕ; h, θ) ≈ Gaussian
F. Lavancier () Residuals and GoF tests for Gibbs pp 27/06/2012 10 / 19
The h-residuals Baddeley, Turner, Møller, Hazelton (05)
h−innovations (in Λ) : for any function h(·, ·; θ) : S× Ω→ R,
IΛ(ϕ; h, θ?) :=∑
xm∈ϕΛ
h(xm, ϕ \ xm; θ?)−∫
Λ×Mh(xm, ϕ; θ?)e−V (xm|ϕ;θ?)µ(dxm)
where V (xm|ϕ; θ) := VΛ(ϕ ∪ xm; θ)− VΛ(ϕ; θ) is the local energy of xm in ϕ.
h−residuals (in Λ) : RΛ(ϕ; h, θ) := IΛ(ϕ; h, θ)
Theoretical Motivation :
Theorem (Georgii-Nguyen-Zessin)
For any h(·, ·; θ) : S× Ω→ R, for any θ ∈ Θ,
Eθ?
(∑xm∈ϕ
h (xm, ϕ \ xm; θ)
)= Eθ?
(∫Rd×M
h (xm, ϕ; θ) e−V (xm|ϕ;θ?)µ(dxm)
)
Conjecture from BTMH : RΛ(ϕ; h, θ) ≈ 0 and |Λ|1/2RΛ(ϕ; h, θ) ≈ Gaussian
F. Lavancier () Residuals and GoF tests for Gibbs pp 27/06/2012 10 / 19
The h-residuals Baddeley, Turner, Møller, Hazelton (05)
h−innovations (in Λ) : for any function h(·, ·; θ) : S× Ω→ R,
IΛ(ϕ; h, θ?) :=∑
xm∈ϕΛ
h(xm, ϕ \ xm; θ?)−∫
Λ×Mh(xm, ϕ; θ?)e−V (xm|ϕ;θ?)µ(dxm)
where V (xm|ϕ; θ) := VΛ(ϕ ∪ xm; θ)− VΛ(ϕ; θ) is the local energy of xm in ϕ.
h−residuals (in Λ) : RΛ(ϕ; h, θ) := IΛ(ϕ; h, θ)
Theoretical Motivation :
Theorem (Georgii-Nguyen-Zessin)
For any h(·, ·; θ) : S× Ω→ R, for any θ ∈ Θ,
Eθ?
(∑xm∈ϕ
h (xm, ϕ \ xm; θ)
)= Eθ?
(∫Rd×M
h (xm, ϕ; θ) e−V (xm|ϕ;θ?)µ(dxm)
)
Conjecture from BTMH : RΛ(ϕ; h, θ) ≈ 0 and |Λ|1/2RΛ(ϕ; h, θ) ≈ Gaussian
F. Lavancier () Residuals and GoF tests for Gibbs pp 27/06/2012 10 / 19
Examples of residuals
RΛ(ϕ; h, θ) :=∑
xm∈ϕΛ
h(xm, ϕ \ xm; θ)−∫
Λ×Mh(xm, ϕ; θ)e−V(xm|ϕ;bθ)µ(dxm)
1 Raw residuals : h(xm, ϕ; θ) := 1
2 Inverse residuals : h(xm, ϕ; θ) := eV (xm|ϕ;θ)
3 Pearson residuals : h(xm, ϕ; θ) := eV (xm|ϕ;θ)/2
4 Residuals based on the empty space function :
For r > 0, the choice hr (xm, ϕ, θ) := eV (xm|ϕ;θ)1||xm−ϕ||<r leads to
RΛ(ϕ; hr , θ) = FParam(r)− FNonParam(r)
where F (r) := P (ϕ ∩ B(0, r) 6= ∅) is the empty space function.
F. Lavancier () Residuals and GoF tests for Gibbs pp 27/06/2012 11 / 19
Examples of residuals
RΛ(ϕ; h, θ) :=∑
xm∈ϕΛ
h(xm, ϕ \ xm; θ)−∫
Λ×Mh(xm, ϕ; θ)e−V(xm|ϕ;bθ)µ(dxm)
1 Raw residuals : h(xm, ϕ; θ) := 1
2 Inverse residuals : h(xm, ϕ; θ) := eV (xm|ϕ;θ)
3 Pearson residuals : h(xm, ϕ; θ) := eV (xm|ϕ;θ)/2
4 Residuals based on the empty space function :
For r > 0, the choice hr (xm, ϕ, θ) := eV (xm|ϕ;θ)1||xm−ϕ||<r leads to
RΛ(ϕ; hr , θ) = FParam(r)− FNonParam(r)
where F (r) := P (ϕ ∩ B(0, r) 6= ∅) is the empty space function.
F. Lavancier () Residuals and GoF tests for Gibbs pp 27/06/2012 11 / 19
Asymptotic frameworksAim : asymptotic behavior of the residuals, i.e. as Λ→ Rd
RΛ(ϕ; h, θ) ≈ 0 and |Λ|1/2RΛ(ϕ; h, θ) ≈ Gaussian
In 2 frameworks :
1. computed for different test functions ⇒ joint behavior in law
2. computed on several disjoint sub-domains ⇒ joint behavior in law
=⇒ Construction of Goodness of Fit Tests.
Main assumptions :
Existence and stationarity of Pθ, for all θ ∈ Θ
Locality assumption : ∃D > 0, V (xm|ϕ) = V (xm|ϕB(x,D))
Some regularity assumptions on V and h
For θ an estimate of θ? computed on Λ :
as |Λ| → Rd ,
θ
a.s.−→ θ?
|Λ|1/2(θ − θ?)d−→ T for some r.v. T
F. Lavancier () Residuals and GoF tests for Gibbs pp 27/06/2012 12 / 19
Asymptotic frameworksAim : asymptotic behavior of the residuals, i.e. as Λ→ Rd
RΛ(ϕ; h, θ) ≈ 0 and |Λ|1/2RΛ(ϕ; h, θ) ≈ Gaussian
In 2 frameworks :
1. computed for different test functions ⇒ joint behavior in law
2. computed on several disjoint sub-domains ⇒ joint behavior in law
=⇒ Construction of Goodness of Fit Tests.
Main assumptions :
Existence and stationarity of Pθ, for all θ ∈ Θ
Locality assumption : ∃D > 0, V (xm|ϕ) = V (xm|ϕB(x,D))
Some regularity assumptions on V and h
For θ an estimate of θ? computed on Λ :
as |Λ| → Rd ,
θ
a.s.−→ θ?
|Λ|1/2(θ − θ?)d−→ T for some r.v. T
F. Lavancier () Residuals and GoF tests for Gibbs pp 27/06/2012 12 / 19
Asymptotic frameworksAim : asymptotic behavior of the residuals, i.e. as Λ→ Rd
RΛ(ϕ; h, θ) ≈ 0 and |Λ|1/2RΛ(ϕ; h, θ) ≈ Gaussian
In 2 frameworks :
1. computed for different test functions ⇒ joint behavior in law
2. computed on several disjoint sub-domains ⇒ joint behavior in law
=⇒ Construction of Goodness of Fit Tests.
Main assumptions :
Existence and stationarity of Pθ, for all θ ∈ Θ
Locality assumption : ∃D > 0, V (xm|ϕ) = V (xm|ϕB(x,D))
Some regularity assumptions on V and h
For θ an estimate of θ? computed on Λ :
as |Λ| → Rd ,
θ
a.s.−→ θ?
|Λ|1/2(θ − θ?)d−→ T for some r.v. T
F. Lavancier () Residuals and GoF tests for Gibbs pp 27/06/2012 12 / 19
Asymptotic frameworksAim : asymptotic behavior of the residuals, i.e. as Λ→ Rd
RΛ(ϕ; h, θ) ≈ 0 and |Λ|1/2RΛ(ϕ; h, θ) ≈ Gaussian
In 2 frameworks :
1. computed for different test functions ⇒ joint behavior in law
2. computed on several disjoint sub-domains ⇒ joint behavior in law
=⇒ Construction of Goodness of Fit Tests.
Main assumptions :
Existence and stationarity of Pθ, for all θ ∈ Θ
Locality assumption : ∃D > 0, V (xm|ϕ) = V (xm|ϕB(x,D))
Some regularity assumptions on V and h
For θ an estimate of θ? computed on Λ :
as |Λ| → Rd ,
θ
a.s.−→ θ?
|Λ|1/2(θ − θ?)d−→ T for some r.v. T
F. Lavancier () Residuals and GoF tests for Gibbs pp 27/06/2012 12 / 19
Asymptotic frameworksAim : asymptotic behavior of the residuals, i.e. as Λ→ Rd
RΛ(ϕ; h, θ) ≈ 0 and |Λ|1/2RΛ(ϕ; h, θ) ≈ Gaussian
In 2 frameworks :
1. computed for different test functions ⇒ joint behavior in law
2. computed on several disjoint sub-domains ⇒ joint behavior in law
=⇒ Construction of Goodness of Fit Tests.
Main assumptions :
Existence and stationarity of Pθ, for all θ ∈ Θ
Locality assumption : ∃D > 0, V (xm|ϕ) = V (xm|ϕB(x,D))
Some regularity assumptions on V and h
For θ an estimate of θ? computed on Λ :
as |Λ| → Rd ,
θ
a.s.−→ θ?
|Λ|1/2(θ − θ?)d−→ T for some r.v. T
F. Lavancier () Residuals and GoF tests for Gibbs pp 27/06/2012 12 / 19
Framework 1 ((h1, . . . , hs)−residuals on Λ))8>>>>>>>>>><>>>>>>>>>>:
RΛ(ϕ, h1, bθ)
.
.
.
RΛ(ϕ, hj , bθ)
.
.
.
RΛ(ϕ, hs , bθ)
Take s different test-functions hj
Compute each hj -residuals from Λ
Consider the vector R1 :=(
RΛ(ϕ, hj , θ))
j=1,...,s.
Theorem (Coeurjolly, L.)
|Λ|−1R1a.s.→ 0 and |Λ|−1/2 R1
d→ N (0,Σ1), as Λ→ Rd ,
where Σ1 is a matrix depending on h, V and the asymptotic behavior of θ
Corollary (Empty space function type test)
Test 1 : Under some conditions ensuring Σ1 positive-definite
|Λ|−1 ‖Σ−1/21 R1‖2 d→ χ2
s ,
where Σ1 is a ”natural” estimate of Σ1
F. Lavancier () Residuals and GoF tests for Gibbs pp 27/06/2012 13 / 19
Framework 1 ((h1, . . . , hs)−residuals on Λ))8>>>>>>>>>><>>>>>>>>>>:
RΛ(ϕ, h1, bθ)
.
.
.
RΛ(ϕ, hj , bθ)
.
.
.
RΛ(ϕ, hs , bθ)
Take s different test-functions hj
Compute each hj -residuals from Λ
Consider the vector R1 :=(
RΛ(ϕ, hj , θ))
j=1,...,s.
Theorem (Coeurjolly, L.)
|Λ|−1R1a.s.→ 0 and |Λ|−1/2 R1
d→ N (0,Σ1), as Λ→ Rd ,
where Σ1 is a matrix depending on h, V and the asymptotic behavior of θ
Corollary (Empty space function type test)
Test 1 : Under some conditions ensuring Σ1 positive-definite
|Λ|−1 ‖Σ−1/21 R1‖2 d→ χ2
s ,
where Σ1 is a ”natural” estimate of Σ1
F. Lavancier () Residuals and GoF tests for Gibbs pp 27/06/2012 13 / 19
Framework 1 ((h1, . . . , hs)−residuals on Λ))8>>>>>>>>>><>>>>>>>>>>:
RΛ(ϕ, h1, bθ)
.
.
.
RΛ(ϕ, hj , bθ)
.
.
.
RΛ(ϕ, hs , bθ)
Take s different test-functions hj
Compute each hj -residuals from Λ
Consider the vector R1 :=(
RΛ(ϕ, hj , θ))
j=1,...,s.
Theorem (Coeurjolly, L.)
|Λ|−1R1a.s.→ 0 and |Λ|−1/2 R1
d→ N (0,Σ1), as Λ→ Rd ,
where Σ1 is a matrix depending on h, V and the asymptotic behavior of θ
Corollary (Empty space function type test)
Test 1 : Under some conditions ensuring Σ1 positive-definite
|Λ|−1 ‖Σ−1/21 R1‖2 d→ χ2
s ,
where Σ1 is a ”natural” estimate of Σ1
F. Lavancier () Residuals and GoF tests for Gibbs pp 27/06/2012 13 / 19
Framework 2 (h−residuals on subdomains of Λ)
Λ is splitted in a finite number of sub-domains :
Λ = ∪j∈JΛj , where |Λi | = |Λj |, ∀i , j .
Consider the vector of residuals
R2 :=(
RΛj (ϕ, h, θ))
j∈J.
I the same h in each sub-domainI θ is computed from the whole domain Λ
Theorem (Coeurjolly, L.)
|Λj |−1R2a.s.→ 0 and |Λj |−1/2 R2
d→ N (0,Σ2), as Λ→ Rd ,
where
Σ2 = λInn I|J | + |J |−1(λRes − λInn) J (J = eeT , e = (1, . . . , 1)T ),
λInn ≥ 0 is a covariance depending on h and V ,
λRes ≥ 0 is a covariance depending on h, V and the asympt. behavior of θ.
F. Lavancier () Residuals and GoF tests for Gibbs pp 27/06/2012 14 / 19
Framework 2 (h−residuals on subdomains of Λ)
Λ is splitted in a finite number of sub-domains :
Λ = ∪j∈JΛj , where |Λi | = |Λj |, ∀i , j .
Consider the vector of residuals
R2 :=(
RΛj (ϕ, h, θ))
j∈J.
I the same h in each sub-domainI θ is computed from the whole domain Λ
Theorem (Coeurjolly, L.)
|Λj |−1R2a.s.→ 0 and |Λj |−1/2 R2
d→ N (0,Σ2), as Λ→ Rd ,
where
Σ2 = λInn I|J | + |J |−1(λRes − λInn) J (J = eeT , e = (1, . . . , 1)T ),
λInn ≥ 0 is a covariance depending on h and V ,
λRes ≥ 0 is a covariance depending on h, V and the asympt. behavior of θ.
F. Lavancier () Residuals and GoF tests for Gibbs pp 27/06/2012 14 / 19
Quadrat-counting based tests
Corollary (Coeurjolly, L.)
Test 2 : If λInn > 0 and λRes > 0 then
|Λj |−1 ‖Σ−1/22 R2‖2 d→ χ2
|J |,
with Σ−1/22 = 1√bλInn
I|J | + ( 1√bλRes
− 1√bλInn
)J,
where λInn and λRes are “natural” estimates of λInn and λRes .
Test 3 : If λInn > 0 then
|Λj |−1 λ−1Inn × ‖R2 − R2‖2 d→ χ2
|J |−1,
where λInn is a “natural” estimates of λInn.
F. Lavancier () Residuals and GoF tests for Gibbs pp 27/06/2012 15 / 19
Quadrat-counting based tests
Corollary (Coeurjolly, L.)
Test 2 : If λInn > 0 and λRes > 0 then
|Λj |−1 ‖Σ−1/22 R2‖2 d→ χ2
|J |,
with Σ−1/22 = 1√bλInn
I|J | + ( 1√bλRes
− 1√bλInn
)J,
where λInn and λRes are “natural” estimates of λInn and λRes .
Test 3 : If λInn > 0 then
|Λj |−1 λ−1Inn × ‖R2 − R2‖2 d→ χ2
|J |−1,
where λInn is a “natural” estimates of λInn.
F. Lavancier () Residuals and GoF tests for Gibbs pp 27/06/2012 15 / 19
ConclusionTest 1 : different test functions (h1, . . . , hs) in the same domain
|Λ|−1 ‖Σ−1/21 R1‖2 d→ χ2
s ,
−→ deep goodness of fit assessment through (h1, . . . , hs)
−→ Σ1 is a full matrix : not easy to estimate, Σ−1/21 could be very instable.
−→ Σ1 depends on the asymptotic behavior of θn
Test 2 : h-residuals computed on |J | sub-domains
|Λj |−1 ‖Σ−1/22 R2‖2 d→ χ2
|J |,
−→ Σ−1/22 = 1√bλInn
I|J | + ( 1√bλRes
− 1√bλInn
)J is explicit.
−→ λRes depends on the asymptotic behavior of θn.−→ condition λRes > 0 could be restrictive and not easy to check.
Test 3 : h-residuals computed on |J | sub-domains
|Λj |−1 λ−1Inn × ‖R2 − R2‖2 d→ χ2
|J |−1.
−→ λInn > 0 easy to check and not restrictive.
−→ Generalization of the Poisson dispersion test.F. Lavancier () Residuals and GoF tests for Gibbs pp 27/06/2012 16 / 19
Short simulation in the simplest case : quadrat test (Test 3) with h = 1
True model : Strauss model on Λ = [0, L]2
VΛ(ϕ; θ) = θ1|ϕΛ|+ θ2
∑(x ,y)∈ϕΛ
1||y−x ||<R
In blue : Estimated level of the test when the I-type error is 5%
→ Based on 500 realisations and |J | = 4 or |J | = 9 sub-domains
|J | = 4 |J | = 9L = 1 L = 2 L = 3 L = 1 L = 2 L = 3
Strauss model, R = .05e−θ1 = 200, e−θ2 = 1 6.3% 6% 5.5% 5.8% 5.8% 5.6%
e−θ1 = 300, e−θ2 = 0.3 4.8% 5.4% 5.0% 4.0% 4.8% 5.4%e−θ1 = 300, e−θ2 = 0.7 4.8% 5.0% 5.4% 4.4% 4.5% 5.5%
Inhomogeneous Strauss model, R = .05e−θ1 = 300β(·), e−θ2 = 0.3 12.0% 68.4% 100.0% 9.0% 68.2% 100.0%
Neymann-Scott processρ = 30, r = .6 20.2% 36.2% 38.2% 19.6% 45.0% 51.8%ρ = 30, r = .2 53.8% 56.2% 57.8% 65.4% 83.8% 86.2%
Pairwise step function, (R1,R2) = (.06, .1)e−θ1 = 500, e−θ2 = .3, e−θ3 = .7 1.6% 2.4% 3.0% 1.0% 2.8% 2.8%e−θ1 = 500, e−θ2 = .7, e−θ3 = .3 3.2% 4.2% 5.2% 2.8% 5% 4.4%
F. Lavancier () Residuals and GoF tests for Gibbs pp 27/06/2012 17 / 19
A. Baddeley, R. Turner, J. Møller and M. Hazelton, (2005) Residualanalysis for spatial point processes, J.R.S.S. B, 65, 617-666.
J.-F. Coeurjolly, F. Lavancier, (2012) Residuals and Goodness-of-fittests for stationary marked Gibbs point processes, to appear inJ.R.S.S. B (arXiv :1002.0857).
F. Lavancier () Residuals and GoF tests for Gibbs pp 27/06/2012 18 / 19
Theoretical Ingredient
Theorem (Coeurjolly, L.)
Let Xn,i , n ∈ N, i ∈ Zd , be a triangular array field in a measurable space S. Forn ∈ N, let Kn ⊂ Zd and for k ∈ Kn, assume
Zn,k = fn,k (Xn,k+i , i ∈ I0) ,
where I0 = i ∈ Zd , |i | ≤ 1 and fn,k : SI0 → Rp. Let Sn =∑
k∈KnZn,k . If
(i) c3 := supn∈N supk∈KnE|Zn,k |3 <∞,
(ii) ∀n ∈ N, ∀k ∈ Kn, E(Zn,k |Xn,j , j 6= k) = 0,
(iii) |Kn| → +∞ as n→∞,
(iv) There exists a symmetric matrix Σ ≥ 0 such that
E
∥∥∥∥∥∥|Kn|−1∑k∈Kn
∑j∈Bk (1)∩Kn
Zn,kZn,jT − Σ
∥∥∥∥∥∥→ 0,
then |Kn|−1/2Snd−→ N (0,Σ) as n→∞.
F. Lavancier () Residuals and GoF tests for Gibbs pp 27/06/2012 19 / 19