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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

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