Geoscience Reference
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Box 12.4: Hermite Polynomials
p
j
j ð 2 u j 2
j ðÞ
2 2
u j
u j 4
Hermite polynomials H j ( u ) satisfy
H j u
ðÞ ¼
þ
2 !
j ðÞ
2 3
u j 6
,wh e j ( t )
þ ...
¼
j ( j
1)( j
2)
...
( j
t + 1). For
example:
3
!
u 2
u 3
u 4
6 u 2 +3;
H 0 ( u )
¼
1; H 1 ( u )
¼
u ; H 2 ( u )
¼
1;
H 3 ( u )
¼
3u; H 4 ( u )
¼
10 u 3 +15 u .If Z 1 and Z 2 are two standard normal random variables
with zero means, unit variances and correlation coefficient
u 5
H 5 ( u )
¼
ˁ
, their bivariate
½
ð
Þ = 21 ˁ
ð
Þ
½
ð
Þ
exp z 1 2 ˁz 1 z 2 þz 2
2
exp ½ z 1 þz 2
p
1 ˁ
density function is:
ˆ
ð
z 1 ;
z 2
Þ ¼
¼
2 ˀ
2 ˀ
2
h
i representing the Mehler identity. Other properties
X j ¼1 ˁ
j H j zðÞ
1
þ
H j zðÞ
j where X is a normal random variable with mean
include E { H j ( X )}
¼ ʼ
ʼ
.
X 2 .
If f ( x 1 ) and f ( x 2 ) are of the same type, their frequency distribution is permanent.
Examples include the lognormal and logbinomial distributions. Permanence of
these two distributions was first established by Matheron ( 1974 , 1980 ). It means
that blocks of different sizes have the same type of frequency distribution; for
example, all can be lognormals with the same mean but different logarithmic
variances.
The regression of X 1 on X 2 ,or E ( X 1 | X 2 )
When f ( x 1 ) is known, f ( x 2 ) can be derived in combination with E ( X 1 | X 2 )
¼
¼
X 2 , results in the following two
relations between block variances:
2 XðÞ ¼ σ
2 X 1
2 Xð ; σ
2 XðÞ ¼ ˁ
2
2 XðÞ
σ
ð
X 2
Þ þ σ
x σ
with
0 representing the product-moment correlation coefficient of X 1 and X 2 .
The first part of this equation can be rewritten as
ˁ x >
2 ( V ). Suppose
that v is contained within a larger volume v' that, in turn, is contained within V .
Then,
2 ( v , V )
2 ( v )+
σ
¼ σ
σ
2 ( v 0 , V ) These results are general in that they do not
only apply to original element concentration values but also to transformed element
concentration values; e.g. E (ln X 1 |ln X 2 )
2 ( v , V )
2 ( v, v 0 )+
σ
¼ σ
σ
ln X 2 . The resulting logarithmic
variance relationship for average values in blocks of three different sizes was
originally discovered by Krige ( 1951 ) and was called “Krige's formula for the
propagation of variances” by Matheron (Sect. 2.1.2 ) .
This result also can be derived as follows. Using Hermite polynomials the
lognormal
¼
random variable
X 1
can
be
written
as
X 1 ¼ ʼ
exp
j
1 H j ( Z 1 )/ j !. From results for correlation between X 1 and
X 2 described in Box 12.5 it follows that X 2 satisfies the same expression when σ 1 is
replaced by
1 )
¼ ʼ j ¼ 0 σ
(
σ 1 Z 1 ½ σ
2
2
.
It is possible to use the relation
σ 2 , and
σ
2 ¼ σ
1 ˁ
2 (ln X 2 ) to estimate the correla-
tion coefficient ˁ x . The following example of application was described in
Agterberg ( 1977 ). Probability indices for occurrence of large copper deposits in
2 (ln X 1 )
2
σ
¼ ˁ
x σ
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