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hand side of the equation, with the kernel defined by Green's function of the
differential operator
PP
ˆ
PPG x x
(, )
G .
(
x
x
)
i
i
Bearing in mind the definition of Green's function and taking into account the
presence of the delta function on the right-hand side of the equation, the integral
transformation will generate a discrete sum of terms, so that the function
f
can be
defined as
1
n
fx
()
¦
(
y
fx Gxx
( )) (, )
,
i
i
i
O
i
1
where
G
(
x
,
x
i
) is
Green's function
centred at
x
i
. The last equation represents the
solution of the regularization problem as a linear combination of
n
Green's
functions with the expansion centre
x
i
and expansion coefficients (
y
i
í
f
(
x
i
)).
Consequently, the solution of the regularization problem lies in the
n
-dimensional
subspace of the space of smooth functions, with the
n
Green's functions as its basis
(Poggio and Girosi, 1990). Furthermore, the basis function depends on stabilizer
P
,
that represents the
a priori
knowledge of the problem domain as a kind of
constraint.
Introducing the definition of the expansion weights as
yf
()
x
w
i
i
,
i
O
the above solution equation becomes
n
f
()
x
¦
Gx x
(, )
.
i
i
i
1
w
, the last two equations have to be
Now, to determine the expansion weights
written in matrix form as
1
(
wy
f
)
O
and
f
Gw
which result in
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