Studio delle prestazioni di un sistema a fosfori per mammografia ...
Studio delle prestazioni di un sistema a fosfori per mammografia ...
Studio delle prestazioni di un sistema a fosfori per mammografia ...
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where £ is the system gain.<br />
The PSF has a f<strong>un</strong>ctional form identical to that of the image generated by a Æ-pulse input. If<br />
the system is space invariant, a point-source input can be moved along the object plane without<br />
any effect other than changing the location of its image, the f<strong>un</strong>ction being the same for any<br />
point Ü� Ý . So the dependence of the PSF on space variables can only be related to Ü� Ý as<br />
far as the location of its center is concerned. The value of the PSF on the image plane merely<br />
depends on the <strong>di</strong>splacement at that location from the particular image point at which the PSF<br />
is centered (see Fig. 2.1).<br />
Figure 2.1: Convolution of a source composed of Æ f<strong>un</strong>ctions with the PSF. The resulting pattern<br />
is the sum of all the spread out contributions.<br />
In other words it can be stated that:<br />
ÈË� Ü� Ý� �� � �ÈË� � Ü� � Ý (2.5)<br />
then, <strong>un</strong>der the hypotheses of space invariance and linearity,<br />
� �� � �£<br />
��<br />
� Ü� Ý ÈË� � Ü� � Ý �Ü�Ý (2.6)<br />
It is also worth defining the Line Spread F<strong>un</strong>ction (LSF) as the integral of the PSF along<br />
one <strong>di</strong>rection, since this is the quantity that will be used to ex<strong>per</strong>imentally evaluate the spatial<br />
17