• Non ci sono risultati.

View of Some properties of Kemp family of distributions

N/A
N/A
Protected

Academic year: 2021

Condividi "View of Some properties of Kemp family of distributions"

Copied!
6
0
0

Testo completo

(1)

SOME PROPERTIES OF KEMP FAMILY OF DISTRIBUTIONS C. Satheesh Kumar

1. INTRODUCTION

Kemp (1968) considered a wide class of univariate discrete distributions called the generalized hypergeometric probability distributions (GHPD), which has the following probability generating function (p.g.f.).

( ; ; ) ( ) ( ; ; ) p q p q F a b t G t F a b    (1)

where p qF a b( ; ; ) is the generalized hypergeometric series (cf. Slater, 1966 and Mathai and Saxena, 1973) , in which a ’ s, b’s and  are assumed to be appropri-ate reals and the domain of G(.) is an open interval containing the region of con-vergence of p qF a b( ; ; ) . (Dacey, 1972) has listed more than fifty p.g.f.’s involving the generalized hypergeometric series, in which more than twenty are special cases of (1). These special cases include several well-known discrete distributions such as binomial, Poisson, negative binomial, hypergeometric, inverse hyper-geometric, negative hyperhyper-geometric, Polya, inverse Polya, Waring, Yule etc. (Kemp, 1968) has studied the properties of the GHPD by considering certain dif-ferential equations satisfied by various generating functions of the GHPD. For a detailed account of GHPD see (Johnson et al., 2005). (Moothathu and Kumar, 1997) introduced and studied a bivariate version of GHPD and (Kumar, 2002, 2009) introduced extended versions of GHPD.

Here in section 2 we show that all the moments of the GHPD exists finitely and obtain an expression for raw moments of the GHPD. In section 3 we derive certain useful and simple recurrence relations for probabilities, raw moments and factorial moments of the GHPD.

Throughout the paper let us adopt the following simplifying notations, for i = 0, 1, ... .

( ; ; )

i p q p q

(2)

1 1 ( ) ( ) p j j n i q k k n a i D b i       

and ( )a  ( )0 1, a n a a( 1)...(a n 1),n Further we need the following se-1. ries representation in the sequel.

0 0 0 0 ( , ) r ( , ) r s r s B s r B s r s         





(2) 2. MOMENTS OF GHPD

Let X be a random variable having GHPD with the following p.g.f., in which

for r  , ( ; )0 P a brP X r(  denote its probability mass function. )

0 ( ) ( ; ) r r r G tP a b t  

1 0 p q( ; ; ) HF a b t  (3)

Now we have the following result.

Result 2.1 For any positive integer r , the r -th raw moment r of GHPD exists finitely.

Proof. In (3),  < 1 when p q  . Then for 1   0, for any positive integer r and for any t in (-1, 1), ( )r ( ) r ( )

r

d G t

G t

dt

 exists and is continuous. When

p q and/or when = 0, obviously G( )r ( )t exists and is continuous at every

real number t . Thus G( )r ( )t exists and is continuous for every t in an open in-terval containing unity. Hence the r -th factorial moment of GHPD is

[ ] [ ]r E X( r )   ( ) 1 [ r ( )] t G t   1 1 0 ( ) ...( ) ( ) ...( ) r r p r r r q r a a H b b H   ,

which is finite, since p qF a b( ; ; ) in (3) is assumed to be convergent. From (John-son et al., 2005) we have

(3)

[ ] 0 ( , ) r r j j S r j    

(4)

where ( , )S r j are the Stirling numbers of the second kind. Hence ( r)

r E X

 

exists finitely.

Here onwards we shall denote r r( ; )a b . Therefore the characteristic func-tion 1 0 ( )t G e( )it H p qF a b e( ; ; it)    (5) 0 ( ) ( ; ) ! r r r it a b r    

(6)

On expanding p qF(.) and the exponential function e in (5) we have the follow-it

ing. 1 1 0 0 1 0 ( ) ( ) ( ) ! ! ( ) p n r j j n q n k k n r a nit t H n r b            

(7)

Equating coefficients of ( !) ( )r 1 it r on right hand side expressions of (6) and (7) we get 1 1 0 0 1 ( ) ( ; ) ! ( ) p n j j n r r q n k k n a a b H n n b          

01 1 0 1 0 ( ) ( , )( ) ! ( ) p n r j j n m q n k k n m a H S r m n n b          

,

where ( , )S r m are the Stirling numbers of the second kind. Writing

! ( ) (m )!

nn n m and rearranging the terms, we obtain

1 1 0 0 0 1 ( ) ( ; ) ( , ) ( )! ( ) p n m r j j n m r q m n k k n a a b H S r m n m b              

01 1 0 0 1 ( ) ( , ) ! ( ) p n r j j n m m q m n k k n m a H S r m n b             

(4)

1 1 0 0 1 ( ) ( ; ) ( , ) ( ) p r j j m m r q m m k k m a a b H S r m H b         

(8)

which is a simple expression for raw moments of GHPD. 3. RECURRENCE RELATIONS

Result 3.1. The following is a recurrence relation for probabilities of GHPD, for

0 n  . 0 1 1 0 ( ; ) ( 1 ; 1 ) ( 1) n n p q D H P a b P a b n H      (9)

Proof. Consider the following identity obtainable from (3) on differentiation with

respect to t . 1 0 ( ) ( 1) ( ; ) r r r G t r P a b t t      

 0 0 ( 1 ; 1 ; ) p q p q D F a b t H    (10)

In (3) on replacing ,a b by a1 ,p b respectively, we obtain 1q

1 0 ( 1 ; 1 ; ) ( 1 ; 1 ) r p q p q r p q r F a bt HP a b t    

  . (11) By using (11) in (10) we obtain 0 1 0 0 0 ( 1) ( ; )r r r( 1 ;p 1 )q r r r D H r P a b t P a b t H         

.

Equating coefficients of t on both sides, we get the relation (9). n

Result 3.2. The following is a recurrence relation for raw moments of GHPD, for

0 n  , in which 0( ; ) 1a b  . 0 1 0 0 ! ( ; ) ( 1 ; 1 ) !( )! n n 1 n s p q s D H n a b a b H s n s       

(12)

Proof. Consider the following identity obtainable from (5) and (6) on

(5)

it 0 0 e ( ) ( 1 ; 1 ; it) p q p q i D t F a b e t H         1 ( ) ( ; ) ! r r r it r i a b r    

By using (5) and (6) with ,a b replaced by a1 ,p b , one has 1q

0 1 1 0 0 0 ( ) ( ) ( ; ) ( 1 ; 1 ) ! ! r r it r r p q r r D H it it a b e a b r H r           

0 1 0 0 0 ( ) ( 1 ; 1 ) ! ! r s r p q r s D H it a b H r s        



  0 1 0 0 0 ( ) ! ( 1 ; 1 ) !( )! ! r r r s p q r s D H r it a b H s r s r         



,

in the light of (2). On equating coefficients of ( !) ( )n 1 it n on both sides, we obtain (12).

Result 3.3. Let [ ]n( ; )a b denote the n-th factorial moment of GHPD with p.g.f. (3). Then the following is a recurrence relation for factorial moments of GHPD for n  , in which 0 [ 0]( ; ) 1.a b  0 1 [ 1] [ ] 0 ( ; ) ( 1 ; 1 ) n n p q D H a b a b H       (13)

Proof. The factorial moment generating function ( )F t of GHPD with p.g.f. ( )G t

given in (3)is the following.

1 0 ( ) (1 ) p q[ ; ; (1 )] F t G  t HF a bt [ ] 0 ( ; ) ! r r r t a b r    

(14)

The relation (13) follows on differentiating the above equation with respect to t and equating coefficients of ( !)n 1tn on both sides, in the light of the arguments similar to those in the proof of Result 3.1.

Department of Statistics C. SATHEESH KUMAR

(6)

REFERENCES

M. F. DACEY (1972), A family of discrete probability distributions defined by the generalized

hypergeomet-ric series, “Sankhya”, Series B, 34, pp. 243-250.

N. L. JOHNSON, A. W. KEMP, S. KOTZ (2005), Univariate discrete distributions, John Wiley and Sons,

New York.

A. W. KEMP (1968), A wide class of discrete distributions and the associated differential equations,

“Sankhya”, Series A, 30, pp. 401-410.

C. S. KUMAR (2002), Extended generalized hypergeometric probability distributions, “Statistics and

Probability Letters”, 59, pp. 1-7.

C. S. KUMAR (2009), A new class of discrete distributions, “Brazilian Journal of Probability and

Statistics”, 23, pp. 49-56.

A. M. MATHAI, R. K. SAXENA (1973), Generalized hypergeometric functions with applications in statistics

and physical sciences, Lecture Notes No. 348, Springer, Heidelberg.

T. S. K. MOOTHATHU, C. S. KUMAR (1997), On bivariate generalized hypergeometric probability

distribu-tions, “Journal of the Indian Statistical Association”, 35, pp. 51-59.

L. J. SLATER (1966), Generalized hypergeometric functions, Cambridge University Press,

Cam-bridge.

SUMMARY

Some properties of Kemp family of distributions

This paper studies some important properties of the generalized hypergeometric prob-ability distribution (GHPD) of Kemp (Sankhya-Series A, 1968) by establishing the exis-tence of all the moments of the distribution and by deriving a formula for raw moments. Here we also obtain certain recurrence relations for probabilities, raw moments and facto-rial moments of the GHPD.

Riferimenti

Documenti correlati

A) calcoli per ciascun veicolo presente all’interno dell’array v (che si assuma già inizializzato) il costo dell’ingresso alla zona urbana in base ai costi

• Il presente plico contiene 4 esercizi e deve essere debitamente compilato con cognome e nome, numero di matricola, posizione durante lo scritto (comunicata dal docente).. • Non

Si ipotizzi che gli elementi di una coda siano estratti partendo dal primo valore del vettore che rappresenta la coda, e che la variabile ultimoEstratto indichi se l’ultimo

Scrivere lo sviluppo di MacLaurin per la funzione f (x, y) = sin x sin y, arrestato al secondo

Gli esercizi vanno svolti su questi fogli, nello spazio sotto il testo e, in caso di necessit` a, sul retro.. I fogli di brutta a quadretti non devono

Dal Teorema di Rouché-Capelli, il sistema è risolubile se e soltanto se il rango di A coincide con il rango della matrice completa (in questo caso, entrambi sono uguali a 2). Nel

[r]

Il secondo principio della termodinamica afferma che è sempre possibile, mediante un processo meccanico reversibile, raggiungere uno stato di equilibrio stabili con