ANALYSE MATHÉMATIQUE. - Sur une gé néralisation des polynomes d'Hermite. Note de M.Krawtchouk, transmise par M.  Émile Borel.

M. Krawtchouk. C.R.Acad. Sci. 1929. T.189, No.17. P.620 - 622.




MATHEMATICAL ANALYSIS. - On one generalization of Hermite polynomials. Note 1 by M. Krawtchouk, submitted by M.  Émile Borel.

.

Let's assume that the polynomial ym(x) of the mth degree is defined by the following equalities

�
�
�
�
�
�
�
u-1
�
i = 0 
piyl(xi)ym(xi) = 0(l � m),    = 1  (l = m)
�
�
xi+1-xi = 1,    pi � o,    u-1
�
i = 0 
pi = 1 �
�
.
(1)

Then we have

�
�
�
�
�
xym(x) = m-1ym-1(x)+m0ym(x)+m1ym+1(x)
�
�
mj = u-1
�
i = 0 
pixiym(xi)ym+j(xi) �
�
and the minimum of the expression
Jk(T0,T1,�,Tk-1) = u-1
�
i = 0 
pi[T0y0(xi)+�+Tk-1yk-1(xi)-y(xi)]2    (k � u)
(2)
is equal to
Jk(A0,A1,�,Ak-1) = u-1
�
i = 0 
piy2(xi)-A02-�-AN-12
where
Am = u-1
�
i = 0 
piy(xi)ym(xi).
(3)

In the important case p0 = p1 = � = pu-1 which has been studied by P. Tchebycheff the polynomials ym represent the generalization of the Legendre polynomials. We want to consider other important case where

pi = P(i,u;p,q) = �
�
�
u-1
i
�
�
�
piqu-1-i,    xi = i   (p > 0,  q > 0,  p+q = 1).
(4)

It is possible to prove that the functions ym have according to this hypothesis the following simple form:

jm(x,u;p,q)
=
  �
 �
�

�
�
�
u-1
m
�
�
�
(pq)m
 
  DmP(x-m,u-m;p,q):P(x,u;p,q)
(5)
=
  �
 �
�

�
�
�
u-1
m
�
�
�
-1

 
(pq)-m
 
m
�
i = o 
(-1)i �
�
�
u-x-1
m-i
�
�
�
�
�
�
x
i
�
�
�
pm-iqi
concerning the limiting cases of the polynomials
const. x!
ax
Dm �
�
�
ax-m
(x-m)!
�
�
�
    (u� �),  p(u-1) = a = const.)
(6)
and the Hermite polynomials
const.et2 dm
dtm
( e-t2)     �
�
u� �,  x = p(u-1)+t   _______
�2pq(u-1)
 
�
�
.
(7)

In accordance with (4) the formulas (*) and (3) are conversed respectively to

  ____________
�(m+1)(u-m-1)pq
 
 jm+1(x)
=
[ p(u-1)+(q-p)m-x] jm(x)-   _______
�m(u-m)pq
 
jm-1(x),
Am
=
  �
 �
�

�
�
�
u-1
m
�
�
�
(pq)m
 
u-1
�
i = 0 
y(xi)DmP(xi-m,  u-m;  p,q)
(8)
=
(-1)m   �
 �
�

�
�
�
u-1
m
�
�
�
(pq)m
 
u-1
�
i = 0 
P(i-m,u-m;p,q)Dmy(i-m),

Appendices. - 1. Calculation of the incomplete generalized moments

Rm(x) = x-1
�
i = 0 
P(i,u;p,q)jm(i,u;p,q)    (m = 1,2,�,k)
of function (4) gives
Rm(x) =   �
 �
�

�
�
�
u-1
m
�
�
�
(pq)m
 
Dm-1P(x-m,u-m;p,q)   (m = 1,2,�,k)
(9)

As to kth incomplete factorial moment

rk(x) = x-1
�
i = 0 
P(i,u;p,q) �
�
�
p( u-1) -x
k
�
�
�
   (k = 0,1,2,�),
it is equal to the linear combination of expressions (9) and moment R0(x) [the result is trivial in a limiting case (7)]. Equality by M.R. Frisch2 follows from the formula (9) as a special case at (m = 1).

- 2. It is necessary to note the following expansion

P(x,u1;p1,q1)
=
P(x,u;p,q) u-1
�
m = 0 
  �
 �
�

(u-m-1)!
m!(u-1)!
(pq)-m
 
jm(x,u;p,q)
× m
�
i = 0 
(-1)m-i �
�
�
m
i
�
�
�
pm-iqi �
�
�
dm[su-m(p1t+q1s)u1]
dtidsm-i
�
�
�


s,t = 1 
(u
�
u1),
with the limiting cases which correspond to the polynomials (6) and (7) and are well known.


Footnotes:

1Submitted on September 23, 1929.

2See Ch. Jordan, Statistique math., 1927, p. 85


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