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Research Directory of the Brandenburg University of Applied Sciences

Research Directory of the Brandenburg University of Applied Sciences

Research Directory of the Brandenburg University of Applied Sciences

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Fachhochschule <strong>Brandenburg</strong><br />

<strong>Brandenburg</strong> <strong>University</strong> <strong>of</strong> <strong>Applied</strong> <strong>Sciences</strong><br />

<strong>the</strong> image at a given spatial frequency relative to low frequencies.<br />

For <strong>the</strong> experimental determination <strong>of</strong> <strong>the</strong> MTF<br />

a USAF line pair standard was used. This standard consists<br />

<strong>of</strong> a photolithography mask with line pairs. The line<br />

pairs <strong>of</strong> each frequency are arranged in a 1 mm broad<br />

array on <strong>the</strong> mask. These arrays are splitted by a 300 μm<br />

wide chromium layer. The number <strong>of</strong> line pairs per millimeter<br />

(lp/mm) is in <strong>the</strong> range 5 to 200 lp/mm, see Fig.<br />

3.18. With a similar measurement as described above for<br />

<strong>the</strong> single line <strong>the</strong> spatial frequency dependent contrast<br />

<strong>of</strong> <strong>the</strong> raw signal data in <strong>the</strong> <strong>the</strong>rmogram was analyzed.<br />

Obviously <strong>the</strong> line pr<strong>of</strong>iles across <strong>the</strong> line pair structures<br />

show not only <strong>the</strong> intensity modulation caused by <strong>the</strong><br />

line pairs but additionally a smooth raw signal change<br />

over <strong>the</strong> whole line pair structure. The maximum raw signal<br />

data is observed in <strong>the</strong> middle <strong>of</strong> <strong>the</strong> whole line pair<br />

structure. This also indicates a limited MTF.<br />

The resulting MTF (Fig. 3.18, bottom) was evaluated<br />

according to <strong>the</strong> method described in [4]. It shows that<br />

an accurate temperature determination from <strong>the</strong> raw signal<br />

data becomes very difficult for small objects. For getting<br />

accurate temperature results <strong>the</strong> camera calibration<br />

curve should be measured using <strong>the</strong> same object size.<br />

The spatial frequency dependent MTF has to be analyzed<br />

in more detail. Especially <strong>the</strong> influence <strong>of</strong> <strong>the</strong> chromatic<br />

aberration <strong>of</strong> <strong>the</strong> microscope objective due to<br />

<strong>the</strong> large wavelength region 1.5 to 5 μm has to be investigated.<br />

Probably, monochromatic and shorter wavelength<br />

detection will improve <strong>the</strong> MTF results.<br />

In this paper for object sizes below 1 mm only relative<br />

changes <strong>of</strong> <strong>the</strong> raw signal data are used to characterize<br />

<strong>the</strong> object properties.<br />

10 lp/mm VIS-image 10 lp/mm IR-image 50 lp/mm VIS-image 50 lp/mm IR-image<br />

Fig. 3.18: Determination <strong>of</strong> <strong>the</strong> spatial frequency response<br />

(MTF) <strong>of</strong> <strong>the</strong> SC6000 with <strong>the</strong> microscope<br />

objective. VIS- and IR- images <strong>of</strong> <strong>the</strong> 10 and 50<br />

lp/mm structures (top).<br />

Line pr<strong>of</strong>iles <strong>of</strong> <strong>the</strong> IR raw data signals across <strong>the</strong><br />

lines <strong>of</strong> <strong>the</strong> 10 and <strong>the</strong> 50 lp/mm structures (middle).<br />

Spatial frequency dependent MTF determined from<br />

<strong>the</strong> line-pr<strong>of</strong>ile measurement (bottom).<br />

84 Forschungsbericht <strong>Research</strong> Report 2007 – 2010

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