Image Processing Reference
In-Depth Information
ω
y
|F| 2
ω
ω
x
d 2 , used in the MS estimate. The error is not measured as the shortest
distance between a frequency coordinate
Fig. 10.14. The error,
and the k -axis. This should be contrasted with the
TLS error, which does measure the shortest distance, as shown in Fig. 10.9
ω
tensor, via its minor eigenvector, encodes the direction in which a small translation of
the image causes it the least departure from the original. To see this, we perform the
expansion, i.e., we express the image f at r + k , where the direction k =( k x ,k y ) T
has the unit length, by using the partial derivatives of f at r
f ( r + k )= f ( r )+ k x D x + k y D y f ( r )+ 2
2 k x D x + k y D y 2 f ( r )+
···
(10.58)
Accordingly,
k x D x + k y D y f ( r )= f ( r + k )
f ( r ) (10.59)
is the linear approximation of the difference between the function f ( r ) and its trans-
lated version, f ( r + k ). In consequence,
( k x D x + k y D y f ( r )) 2
(10.60)
is the magnitude of the rate of the change in the direction of k , which can be viewed
as the error rate or resistance rate when translating the image in the direction k .
Integrating this function and using the (Parseval-Plancherel) theorem 7.2, yields
k T
f ( x, y ) 2 dxdy = k T
T f ( x, y ) dxdy k = k T Sk
(10.61)
f ( x, y )
which is the dynamic part of our original error function, e ( k ), because
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