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a
b
Hermite basis functions
2D Hermite basis function
1
0.8
1
0.6
0.4
0.5
0.2
0
0
−0.2
−0.5
−0.4
−1
10
−0.6
5
10
−0.8
0
5
0
−5
−5
−1
−10
−10
−8
−6
−4
−2
0
2
4
6
8
10
y
x
−10
x
Fig. 12.2 ( a ) First five one-dimensional Hermite basis functions ( b ) 2D Neural Network based on
the QHO eigenstates: basis function B 1;2 .x;˛/
According to Eq. ( 12.8 ) the first five Hermite polynomials are:
H 0 .x/ D 1 for D 1;a 1 D a 2 D 0; H 1 .x/ D 2x for D 3;a 0 D a 3 D 0
H 2 .x/ D 4x 2
2 for D 5;a 1 ;a 4 D 0; H 3 .x/ D 8x 3
12x for D 7;a 0 ;a 5 D0
H 4 .x/ D 16x 4
48x 2
C 12 for D 9;a 1 ;a 6 D 0
It is known that Hermite polynomials are orthogonal [ 186 ]. Other polynomials
with the property of orthogonality are: Legendre polynomials, Chebychev polyno-
mials, and Laguerre polynomials [ 215 , 217 ].
12.4
Neural Networks Based on the QHO Eigenstates
12.4.1
The Gauss-Hermite Series Expansion
The following normalized basis functions can now be defined [ 143 ]:
x 2
2 ;kD 0;1;2;
k .x/ D Œ2 k 2
1
2 H k .x/e
(12.9)
where H k .x/ is the associated Hermite polynomial. To succeed multi-resolution
analysis Hermite basis functions of Eq. ( 12.9 ) are multiplied with the scale coeffi-
cient ˛. Thus the following basis functions are derived
ˇ k .x;˛/ D ˛ 2 k 1 x/
(12.10)
 
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