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(1)

Sciences

&

Technologie AN°24, Décembre (2006), pp. 36-40

© Université Mentouri Constantine, Algérie, 2006.

First order autoregressive representation of Markov bi-dimensional chains of 1-order

Reçu le 22/03/2005 – Accepté le 15/12/2006

Abstract

This paper suggests an extension of Lai’s results about the first order autoregressive representation of Markov bi-dimensional chain of 1-order. In the case of markov chain with independent components, we find of course the conditions validating these results for each component.

Keywords: Markov’chains , autoregressive process, spectral density, diagonal development of bivariate distribution

Résumé

Ce papier suggère une extension d'un résultat de Lai à propos de la représentation autorégressive des chaînes de Markov bi-dimenssionnelle d'ordre 1. Dans le cas où les composantes de la chaîne sont indépendantes, nous retrouvons naturellement les conditions validant ces résultats pour chaque composante.

Mots clés: Chaînes de Markov, processus autoregressif, densité spectrale, développement diagonal des distributions bivariées.

2000 Mathematics Subject Classification : 60K05

enerally, a markov chain is not an autoregressive process, except for first order homogeneous, aperiodic and irreducible markov chains at two states {0,1}. However, Lai (1977) has shown that under convenient hypothesis, a first order uni-dimensional markov chain, valued in a finite or non-finite countable set, belong to a first order autoregressives processes class. In this paper, we extend this result to the cases of first order bi-dimensional markov chains valued in

{ 0 , 1 ,..., N }

2. Firstly, we study Lai’s analogue conditions and secondly the case of the bivariate distributions having a diagonal development.

G

M. BOUSSEBOUA F. L. RAHMANI

Département de Mathématique, Université Mentouri Constantine, Algérie

ﺞﺋﺎﺘﻧ ﻢﻴﻤﻌﺗ حﺮﺘﻘﻳ ﻞـــــﻤﻌﻟا اﺪـــــه LAI

ﺺﺨﺗ ﻲﺘﻟا

ﻞــــﻴﺜﻤﺘﺑ AR (1) ﻞـــﺳﻼﺴﻠﻟ Markov

ﺔﺟرﺪﻟا ﻦﻣ 1

.

ﺔــﻠﺴﻠﺳ ﺔﻟﺎﺣ ﻲﻓ Markov

ﺼﺤﺘﻧ ﺔﻠﻘﺘﺴﻣ تﺎﺒآﺮﻣ تاد ﻞ

طوﺮﺸﻟا ﻰﻠﻋ ﺎﻌﺒﻃ

LAI ﺔﺒآﺮﻣ ﻞﻜﻟ ﺔﺒﺴﻨﻟﺎﺑ ﺔﻘﻘﺤﺘﻣ

ﺔــــﻴﺣﺎﺘﻔﻤﻟا تﺎﻤﻠﻜﻟ

ا :

ﻞــــﻴﺜﻤﺗ AR (1) ﻞـــﺳﻼﺴﻠﻟ

ﺔــﻠﺴﻠﺳ Markov

ﺺﺨﻠﻣ

(2)
(3)

First order autoregressive representation of Markov bi-dimensional chains of 1-order

37 1. AR(1) representation of first order

bi-dimensional markov chains

Let

( Z

t

= ( X

t

, Y

t

) : tZ )

be a first order bi- dimensional markov chain valued in

{ 0 , 1 ,..., N }

2. If the

chain

( ) Z

t is stationary, the probabilities

( ) t P ( Z ( ) x y )

p

x,y

=

t

= ,

and the transition probabilities

( ) t P ( Z ( x y ) Z ( ) x y )

p

x,y,x,'y'

=

t+1

= ,' ' /

t

= ,

are independent of time

t

. Let’s set down

P

as the transition probabilities matrix,

P

n its

n

th power

( n ≥ 1 )

and

( )

(

xy

x yN )

= π

,

: 0 ,

π

its stationary

distribution.

We start writing the covariance function

γ

(.) of the chain

( ) Z

t under the form of a matrix product. After that we determine its spectral density which we shall compare to that of autoregressive process.

Proposition 1

Let

( Z

t

= ( X

t

, Y

t

) : tZ )

be a first order bi- dimensional markov chain valued in

{ 0 , 1 ,..., N }

2. If this

chain is stationary, then its covariance matrix γ (.) has the form

( ) n = A [ P

n

1

(N+1)2

. Π ] B , n 0

γ

( ) 1 . 1

where

Π = ( π

.0

, π

.1

, . . . , π

.N

)

with

(

j Nj

)

j

π π

π

.

=

0

, . . . ,

,

1

( 1)2

( 1 , . . ., 1 )

t

N+

=

a vector of (N+1)2

R

and A and B are conveniently chosen matrices.

Proof. Let us set down that the relation

( ) 1 . 1

determines entirely the covariance function

γ () .

and a

simple computation provides us the coefficients of the covariance matrix

γ ( ) n

:

( ) n =

i,j

σ

( ) ( ) ( )

( )

( )

( )

⎪⎪

⎪⎪

∑ − =

∑ − >

+ +

N y x y

x ij ij

j i j i N

y x y

x j j i i nxyxy ij ij

n if y

x y x

n if p

y x y x y x

' ,' ,

, , ,

2 4

' ,' ,

, 2 1 2 1 ,,,'' , ,

0 ,

.

0 .

, . ' '

β α π

β α π

with

( )

( )i j

n

y x j

i

x x y

+

= ⎟⎟⎠

⎜⎜⎝

=⎛

4

0 ,

,

. π ,

α

and

( , ) , , 1 , 2 .

2

0 ,

,

⎟⎟ ⎠ ∀ =

⎜⎜ ⎝

= ⎛

+

n=

y x y

i j

i j

y

x j

i

π

β

Considering then the matrix

⎟⎟⎠

⎜⎜ ⎞

=⎛

. .

1 . 0

. .

1 . 0

' . . . ' '

. . .

N N

A A

A

A A

A A

where

( ) ( ) ( )

( x x x N )

x

A

x.

= . π , 0 π , 1 . . . π ,

,

( ) ( ) ( )

( x x N x N )

A '

x.

= 0 , π , 1 , 2 π , 2 , . . . , π ,

and the matrix

( ) ( ) ( ) ( ) ⎟⎟

⎜⎜ ⎝

= ⎛

+ + + +

N N

N N

B N

N

t N

t N t N

t t

,..., 1 , 0 . . . ,..., 1 , 0 ,..., 1 , 0 ,..., 1 , 0

1 . . . . 1 . 2 1 . 1 1

.

0

1 1 1 1

we verify easily that

( )

( P ) B ( ) n

A .

n

− 1

N+12

. Π . = γ

This is being true for every

n

0

, setting down of course ( 1)2

0

= I

N+

P

the (N+1)²-order unitmatrix.

Proposition 2

Let

( Z

t

: tZ )

be a first order bi-dimensional markov chain with valued in

{ 0 , 1 ,..., N }

2, irreducible, aperiodic and stationary and let be its stationary distribution. If the matrix

P

of transition probabilities of

( Z

t

: tZ )

admits simple and non nul eigenvalues and if one at least of the following conditions

( ) C

is satisfied, then the spectral density of the chain

( Z

t

: tZ )

is given by :

( ) ( ) ( ) 0

cos . 2 1

1 2

1

2 2 2

2

2

γ

π λ

λ z z

f z

− +

= −

( ) 1 . 2

where

z

2 is the secund large eigenvalue (in absolute value) of P

Conditions

( ) C

:

( )

( )( )

( )

( )( )

( )( )

( )( )

⎪ ⎪

⎪⎪

=

=

⎪ ⎪

⎪⎪

= +

= +

=

+ + +

=

+ + +

=

+ + +

=

+ + +

N

y x

y N x j N

y x

y N x j

N

y x

y N x j N

y x

y N x j

v y and v x ii u

y x y and

u y x x i

0 ,

1 1 0 ,

1 1

0 ,

1 1 0

,

1 1

0 .

0 .

) , 0 .

1 , .

0 .

1 , . )

π

π

(4)

( N ) and where u

( )j

and v

( )j

j

=

3 , . . .,

+

1

2

are respectively the eigenvectors of matrices

P

and t

P

associated to the eigenvalue

z

j. Proof.

Taking into account the factorization

( ) 1 . 1

of

γ ( ) n

and that

I − 1

(N+1)2

.

t

Π = γ ( ) 0

is symetrical, we can write the series

∑ ( )

Z n

in

n

e

λ

γ

under the form

( )

[

( )

]

( )

[

( )

]

( )

[

A ( ) B

]

B e e A

B e G A B e G A B I

A n e

N t i N

i

t i i N

Z n

in

. . 1 1 .

. 1 . 1 1 .

1

. . . . . . 1 .

2 2

2

1 1

1

Π

Π

+ +

Π

=

+

+

+

λ λ

λ λ

λγ

( ) 1 . 3

where

G ( ) ( z = Iz . P )

1

: z ≤ 1

is the generating function of the transition probabilities matrix

P

. As

P

is supposed to be simple and its eigenvalues aren’t nul, then following result of Lancaster (1968) and taking into account

( ) C

conditions, we can write :

( )

[ ( ) ] ( ) ( A u v B )

B z v u z A

B z G A and

B v u z A

B v u z A B z G A

t t t t

t

t t

2 2 2 2 1

1

2 2 2 2 1

1

. .

. 1 . . 1

.

. .

. 1 . . 1

.

λ λ λ λ

− −

− −

=

− −

− −

=

where

u

1

= 1

(N+1)2

and v

1

= Π

are the eigenvectors of

P

and t

P

associated to the eigenvalue

2

1

1 and λ

z

= indicate the inverse of the

eigenvalue

z

2 (we shall notice that the vector is solution of the equation Π=Π

. P

because

π

is a stationary distribution). Reporting these expressions in

( ) 1 . 3

, this latter becomes

( ) [

( )

] ( )

(

. . .

) ( )

1.4

. . .

. . 1 .

. 1 . 1 .

. 1 . 1 .

2 2 2 2 2 2 2 2

1 1 1

12 1

B v u e A

B v u e A

B v u e A B v u e A B I

A n e

t t i t i

t t i t

i t

N Z

n in

λ λ λ

λ γ

λ λ

λ λ

λ

− −

− −

− −

− − Π

=

+

The sum of the first three terms on the right hand side of

( ) 1 . 4

is reduced to

AB

(because the matrices

AB

and

( )

B

A

t

N

. .

1

.

2

1

Π

+ are symetrics), and taking into account

( ) C

conditions, we have (Lancaster (1968)) :

Au

2t

v

2

B = ABA . 1

(N+1)2

.

t

Π . B

Substiting these results in relation

( ) 2 . 4

, we obtain :

( ) Au v B

z z

n

t

Z n

n

2 2 2

2

2

1

. λ

γ λ

= −

Now, we deduce the autoregressive representation of the chain

( Z

t

: tZ )

.

Corollary 1

Let

( Z

t

: tZ )

be a first order bi-dimensional markov chain with states in

{ 0 , 1 ,..., N }

2.

If this chain satisfies the conditions in the proposition 2, then this chain is a first order autoregressive and admits as representation

( ) 1 . 5

.

1

1 t t

t

z Z

Z =

+ ε

where

( ε

t

; tZ )

is a sequence of an uncorrelated random variable, having as covariance matrix

Γ

1

= ( 1z

12

) . γ ( ) 0 .

The representation

( ) 1 . 5

allows us to see that the components

X

t

and Y

t of the chain

( ) Z

t satisfy a first order autoregressive equation without being markov chains. This result is then legitimely proved by the fact that if the components

( ) X

t

and ( ) Y

t are stochastically independent, so each component defines a first order markov chain valued in

{ 0 , 1 ,..., N }

2, which are homogeneous, aperiodic and irreducible, and if

2

1

and P

P

are the transition probabilities matrices of

t

t

and Y

X

respectively, then we have

P

=

P

1

P

2 (tensorial product of

P

1

and P

2) and it is easy to see that the covariance matrix

R

is in this case ⎟⎟

⎜⎜ ⎞

2 1

0 0 γ γ

where

γ

1

and γ

2 are the covariance matrices of

( ) X

t

and ( ) Y

t respectively. On the other hand, if

λ

is an eigenvalue of

P

1

and

t

( x

1

, . .. .., x

N+1

)

is an eigenvector associated to

λ

, then the latter is also eigenvalue of

P

associated to the eigenvector

(

1

, . .. ..,

+1

)

=

t

u u

N

u

with

u

j =t

( x

1

, . .. .., x

N+1

)

:

N j = 1 ,...,

, and if

λ

is an eigenvalue of

P

2 and

(

1

, . .. ..,

N+1

)

t

y y

is an eigenvector associated to

λ

, then so

λ

is also an eigenvalue of P associated to the eigenvector

ω =

t

( ω

1

, . .. .., ω

N+1

)

with

ω

j

= y

j

. 1

N+1 :

1 ., . . . ,

1 +

=

j N

. From this, we show that the

conditions

( ) C

are reduced to Lai’s conditions for each chain

( ) X

t

and ( ) Y

t . This confirms the individual autoregressive representation of

( ) X

t

and ( ) Y

t

(5)

First order autoregressive representation of Markov bi-dimensional chains of 1-order

39 02. Diagonal Development

According once more to Lai, let’s suppose that the transition probabilities of a bi-dimensional markov chain

( ) Z

t satisfy the relation

( ) ∑ ( ) ( ) ( )

=

= N

m n

m n m n m n y

x y

x p x y x y x y

p

0 ,

, ,

, '

,' ,

, ,' ' ρ .θ , .θ ,' ' 2.1

where

. ( ) θ

n,m

: n , m ∈ { 0 ,...., N }

is a sequence of orthogonal functions relatively to the law

( ) ( ) { }

{ p x , y = P X

t

= x , Y

t

= y : x , y ∈ 0 ,...., N }

( ) ( ) ( )

⎟⎟

⎜⎜ ⎞

=

=

symbol s

kronec is

y x y

x y

x p e

i

nn mm i j

N

m n

m n m

n

, . , . , ker'

. , .

.

, ' , ' ,

0

,

θ

,

θ

,' '

δ δ δ

and

( ) ρ

n,m is a sequence of parameters caracterizing the bivariate distribution of

( ) Z

t and

( ) Z

t1 which we find directly from

( ) 1 . 4

. We find the following result :

Lemma 1

If the markov chain

( ) Z

t is irreducible and if we suppose

( ) , 1 , ,

1

00

01 10

00

= ρ = ρ = θ x y =

ρ

10

( ) x , y = α

10

x + β

1,0

and θ

01

( ) x , y = α

01

x + β

01

, ∀ x , y ∈ { 0 , 1 ,...., N } and θ

where

α

10

and α

01

, β

10

and β

01 are real constants with

α

10

≠ 0 and β

10

≠ 0 ,

then we have

( Z

t

.

n,m

( ) Z

t

) = 0 ;

E θ

( , ) { ∈ 0 , 1 ,...., } ( ) ( ) ( )

2

− { 0 , 0 , 1 , 0 , 0 , 1 } .

n m N

If the components of the chain are independent, with the same initial law and for each transition

probability admitting a diagonal development, then the chain

( ) Z

t admits an ease to write diagonal development. In reverse, if the transition probabilities of the

bivariate chain admit a diagonal

development and is at independent components and if

( ) x y

n

( ) ( ) x

m

y

m

n

θ θ

θ

,

, = .

and

( )

x y n

( ) ( )

x m y

m

n ρ ρ

ρ , , = . , then the transition probabilities of each chain

( ) X

t

and ( ) Y

t admit a diagonal development.

A markov bi-dimensional chain of which the transition probabilities are of the form

( ) 2 . 1

is necessarily stationary.

Lemma 2

The eigenvalues of

P

are

( ρ

n,m

: n , m = 0 ,..., N )

with for eigenvectors on the right

( ) ( )

(

nm nm

N ) where

nm

( ) j (

nm

( ) j

nm

( N j ) )

m

n

~ ~ 0 , ,...., ,

,...,

~ 0

, ,

, ,

,

,

θ θ θ θ θ

θ = =

and as eigenvectors on the left

( ) ( )

( Q Q N )

Q

nm nm nm

t

, ,

,

,..., ~

~ 0

= where

( ) j ( Q ( ) j Q ( N j ) ) with

Q ~

nm nm

0 , ,....,

nm

,

, ,

,

=

( ) ( )

,

( ) ( ) { }

2

,

x , y p x , y . x , y ; x , y 0 , 1 ,...., N

Q

nm

= θ

nm

∀ ∈

. Moreover

( )

.

.

, 2

0 ,

, nm n m

t N

m n

m

n

Q I

+

=

θ

= Proof.

Let’s set down

( p

x,y,x,'y'

: 0 ≤ x , x ,' y , y ' ≤ N )

the transition probabilities matrix and note

Π

n,m the

( n, m )

th

row :

(

nm nmN nm nmN nm N nmNN

)

m

n, =

p

,,0,0

, .. ., p

,, ,0

, p

,,0,1

, .. ., p

,, ,1

, . .. .. ., p

,,0,

, .. ., p

,, , Π

By using diagonal development

( ) 3 . 1

of the transition probabilities

p

n,m,x,y and orthogonality of the sequence

( θ

n,m

( ) .,. : 0 ≤ n , mN )

, we easily set up without any difficulty that

ρ

n,m is an eigenvalue of

P

associated to the eigenvector

θ

n,m. Similarly, we check that

Q

n,m is an eigenvector of the matrix t

P

associated to the eigenvalue

n,m

ρ

. Let’s show now that

θ

n,m satisfies the dual orthogonality relationship. Let’s note Θ the eigenvectors matrix,

θ

n,m, and let

Θ

1 be its inverse. Let’s set down

( ) ( ) ( ) ( ) ( )

( ) ( )

⎜⎜

=⎛

y x y

x

y x y

x y x y

x y

x

N N N

N N

, ., ..

, , ., . .

. . . , , ., ..

, , , , ., ..

, , ,

, ,

0

1 , 1

, 0 0

, 0

, 0

θ θ

θ θ

θ θ θ

the

( ) x, y

th row vector of Θ and

( ) ( ) ( ) ( )

( ) ( ) ( )

⎜⎜

= ⎛

y x y

x y

x

y x y x y

y x x

N N N

N t N

, .,

..

, , ., . . . . . , , .,

..

, , , , ., ..

, , ,

, ,

0 1

,

1 , 0 0

, 0

, 0

α α

α

α α

α α

the

( ) x, y

th column vector of

Θ

1

.

We have

( ) ( ) ∑ ( ) ( )

=

=

=

N

m n

y y x x m

n m

n

x y x y

y x y x

0 ,

' , ' , ,

,

, . ,' ' .

' ,' .

, α θ α δ δ

θ

Since the sequence

( θ

n,m

( ) .,. )

is

p ( ) .,.

-orthogonal, then the coefficients

α

n,m

( x ,' y ' )

are provided by

α

n,m

( x ,' y ' ) = p ( x ,' y ' ) . θ

n,m

( x ,' y ' )

(6)

for every

x ,' y '

, and so,

( ) ( ) ( )

( ) ( )

( ) ( )

∑ ∑

= =

=

=

N

m n

N

m n

y y x x m

n m

n

m n m

n m

n

y x p y

x p

y x y

x

y x y

x y

x

0

, , 0

' , ' , ,

,

, ,

,

' ,' . '

,'

' ,' .

,

' ,' .

' ,' .

,

δ α δ

θ

α θ

θ

Now, the

( ) x, y

th coefficient of

Π

n,m is

( ) , .

,

( ,' ' ) ( . ,' ' )

,m

x y Q

nm

x y p x y

θ

n , then

( )

.

.

2

0 ,

, ,

0 ,

, n m

N

m n

m n m

n t N

m n

m

n

Q I

+

=

=

= Π

= ∑

θ

Theorem

Let

( ) Z

t be an irreducible markov chain for which the transition probabilities

p

x,y,x,'y' satisfy the diagonal development

( ) 2 . 1

. If the eigenvalues

ρ

n,m are simple

and real and

ρ

0,0

= 1

and if

( )

⎩ ( )

⎨ ⎧

+

=

+

=

1 , 0 1 , 0 1

, 0

0 , 1 0 , 1 0

, 1

. ,

. ,

β α

θ

β α

θ

x y

x

x y

x

, then the process

( ) Z

t is a first order autoregressive process.

Proof.

The required conditions in the lemma 1 and 2 being satisfied, then the

( ) C

conditions of the proposition 2 are also satisfied, and consequently the chain

( ) Z

t is indeniably a first order autoregressive process.

References

1. Brockwell, P. J. and Davis R. A., (1987). Time series : Theory and methods (Springer Verlag).

2. Feller, W., (1968). An introduction to probability theory and its application Vol 1 (John Wiley & sons)

3. Fuller, W.A. (1996). Introduction to Statistical Times series (Wiley Series in Probability and statistics).

4. Lai, C.D.,(1977). First order autoregressive markov processes. Stochastic processes and their applications, 3 1-4.

5. Lancaster, P., (1968.). Theory of matrices (Academic Press).

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Indeed, we will explain why, on the basis of the empirical power, our test procedure performs better than Ljung–Box [4] and Box–Pierce [5] portmanteau tests, and why it

After the study of the monodomain approximation of the equations and a thorough stability and regularity analysis of weak solutions for the full bidomain equations, as contained in

Given a learning task defined by a space of potential examples together with their attached output values (in case of supervised learning) and a cost function over the

Keywords: second order Markov chains, trajectorial reversibility, spectrum of non-reversible Markov kernels, spectral gap, improvement of speed of convergence, discrete