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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wave object � �� � , oscillating with spatial frequencies �� and �� and amplitude � aro<strong>un</strong>d a<br />
constant value �:<br />
� �� � �� ¡ � � � � �� ���<br />
� (2.11)<br />
A highly useful parameter in evaluating the <strong>per</strong>formances of a system is the contrast or modu-<br />
lation Å, defined by:<br />
Å � �Ñ�Ü �Ñ�Ò<br />
�Ñ�Ü �Ñ�Ò<br />
� ��� (2.12)<br />
The image of the object trough the system can be calculated, in the linear space invariant system<br />
approximation, as:<br />
� Ü� Ý �<br />
� �<br />
� �£<br />
� �£<br />
�£<br />
� �<br />
� Ü �� Ý � ¡ � �� � ���� (2.13)<br />
� �<br />
� �<br />
ÈË� Ü �� Ý � � � � � �� ��� ����<br />
ÈË� Ü �� Ý � ����<br />
ÈË� Ü �� Ý � � � � � � � Ü �� � Ý � � � � �Ü ��Ý ���� �£<br />
where £ is the gain of the system. After a change in the integration variables � � Ü � and<br />
� � Ý �, the same expression is:<br />
� Ü� Ý ��£� � � � �Ü ��Ü<br />
� �<br />
ÈË� �� � � � � � �� ��� ���� �£ (2.14)<br />
The integral is the Fourier transform of the PSF and is usually referred to as OTF (Optical<br />
Transfer F<strong>un</strong>ction). The OTF is thus defined as the Fourier transform of the output of a system<br />
which has a delta f<strong>un</strong>ction as its input. The OTF is two-<strong>di</strong>mensional for a two-<strong>di</strong>mensional<br />
image, but for simplicity of nomenclature only the one-<strong>di</strong>mensional case will be considered<br />
here. With a last change of variables �Ü � �� and �Ý � ��, the image � Ü� Ý can be written as:<br />
� � �ÜÜ �ÝÝ<br />
� Ü� Ý ��£ÇÌ� �Ü��Ý �<br />
�£ (2.15)<br />
It appears that the image of a sinusoid is still a sinusoid and, as it could be expected from the<br />
system linearity, with the same spatial frequency of the object; but the amplitude depends both<br />
19