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Dimensional Measurement using Vision Systems - NPL Publications ...

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<strong>Measurement</strong> Good Practice Guide No. 39<br />

condenser. The latter produces a sharp image of the field stop and thus minimises stray<br />

light, which might otherwise reduce image contrast.<br />

Condensers are conventionally designed with sufficient working distance for use with a<br />

standard microscope slide 1 mm in thickness. Glass photomask substrates are typically<br />

1.5 mm or 2.3 mm in thickness and it is important to ensure that condensers used for<br />

illuminating these masks have adequate working distance.<br />

In reflected light microscopy (apart from very low power work) the microscope objective<br />

itself acts as condenser. A beam splitter located above the objective directs light to the<br />

specimen and then after reflection allows the light to pass through to the eyepiece. Under<br />

these conditions of illumination, image contrast can be seriously reduced by back<br />

reflections from the lens surfaces of the objective since spurious light is able to reach the<br />

eyepiece without taking part in the true image forming process in the microscope.<br />

This effect can be reduced by means of antireflection coatings on the lens surfaces and<br />

these are now almost universally applied to microscope optics. With a single layer coating<br />

the reflectance at an air/glass interface is about 1.5 per cent, compared to a figure of 4 per<br />

cent for an uncoated surface. However, by the use of a multi-layer coating, this reflectance<br />

can be reduced to well below 0.5 per cent and multicoated objectives are therefore<br />

particularly recommended for reflected light microscopy.<br />

2.8 COHERENCE<br />

To study image formation in rather more detail than in section 2.1, it is necessary to<br />

introduce the concept of coherence and to consider the difference between temporal and<br />

spatial coherence.<br />

Assuming light to be propagated as a transverse wave motion, a 'perfectly'<br />

monochromatic beam of light can be represented as consisting of a continuous train of<br />

waves, effectively of infinite length. Light from a helium-neon laser possesses an<br />

extremely narrow bandwidth and can be considered to conform reasonably closely to this<br />

model. In contrast, light emitted by more conventional sources, such as discharge and<br />

tungsten lamps, has a much broader bandwidth, even when interference filters are<br />

employed to isolate a narrow spectral range. The emitted wave trains can then be<br />

regarded as having a finite rather than infinite length, with no fixed phase relation existing<br />

between successive wave trains. The length of the wave trains will decrease with<br />

increasing illumination bandwidth.<br />

17

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