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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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<strong>the</strong>se detectors respond much<br />

faster. The detectors are connected<br />

to a read out circuit<br />

(ROIC) for snapshot integration.<br />

The photocurrent generated<br />

by <strong>the</strong> incident photon flux<br />

will be stored in a capacitor<br />

during a user selectable integration<br />

time (or exposure<br />

time). This integration time<br />

will determine <strong>the</strong> time resolution<br />

<strong>of</strong> <strong>the</strong> camera. For <strong>the</strong><br />

SC6000 variable integration<br />

time settings from 9 μs to full<br />

frame time are possible. For<br />

<strong>the</strong> experiment with <strong>the</strong> falling<br />

ball an integration time <strong>of</strong> 1<br />

ms was used, see Fig. 3.13. No<br />

blurring <strong>of</strong> <strong>the</strong> image <strong>of</strong> <strong>the</strong><br />

ball is observed and <strong>the</strong> temperature<br />

<strong>of</strong> <strong>the</strong> ball can be correctly<br />

determined over <strong>the</strong><br />

whole falling distance.<br />

b) Spatial resolution<br />

The spatial resolution <strong>of</strong> <strong>the</strong> <strong>the</strong>rmal imaging system<br />

determines <strong>the</strong> minimum size <strong>of</strong> objects which can be<br />

analyzed. Fig. 3.16 demonstrates that different camera<br />

systems lead to different results when studying miniaturized<br />

objects. A <strong>the</strong>rmal emitter with an area <strong>of</strong> 2.1<br />

mm x 1.8 mm was analyzed with a 320 x 240 pixels MW<br />

THV 550 camera and <strong>the</strong> 640 x 512 pixels SC6000<br />

camera with different optics.<br />

Obviously <strong>the</strong> SC6000 microscope<br />

optics provides <strong>the</strong> best spatial resolution.<br />

As will be shown below a detailed<br />

analysis <strong>of</strong> this structure is only<br />

possible using <strong>the</strong> SC6000 with<br />

microscope optics.<br />

For <strong>the</strong> determination <strong>of</strong> <strong>the</strong> spatial<br />

resolution <strong>of</strong> <strong>the</strong> SC6000 using <strong>the</strong><br />

microscope objective chromium<br />

structures on a photolithography<br />

mask were used. The mask was heated<br />

up and <strong>the</strong> emissivity contrast <strong>of</strong><br />

<strong>the</strong> mask was used for <strong>the</strong> measurement<br />

across a 34 μm line on <strong>the</strong><br />

mask. Compared to <strong>the</strong> visible microscope<br />

image (Fig. 3.17 left, top) <strong>the</strong><br />

Wissenschaftliche Beiträge – Fachbereich Technik<br />

Scientific Articles – Department <strong>of</strong> Engineering<br />

Fig. 3.16: Thermograms <strong>of</strong> a miniaturized infrared emitter (size 2.1 mm x 1.8 mm) in TO-39 housing<br />

from<br />

- MW camera THV 550 (320 x 240 pixels) with a 24° optics (top, left) and an additional close-up lens<br />

(top, right)<br />

- MW camera SC6000 (640 x 512 pixels) with a 25 mm lens (bottom, left) and microscope optics (bottom,<br />

right)<br />

(Region <strong>of</strong> interest is indicated in <strong>the</strong> left <strong>the</strong>rmograms.)<br />

<strong>the</strong>rmogram appears blurred, see Fig. 3.17 left, bottom.<br />

Raw signal data across <strong>the</strong> line were analyzed and a<br />

signal plateau was observed, see Fig. 3.17, right. The<br />

plateau is formed by about 6 pixels. If this number <strong>of</strong><br />

pixels is compared to <strong>the</strong> line width <strong>of</strong> 34 μm one may<br />

conclude that resolution per pixel amounts to around 5<br />

- 6 μm.<br />

The spatial resolution <strong>of</strong> imaging systems is mostly<br />

described by <strong>the</strong> modulation transfer function MTF [2 -<br />

4]. The MTF is defined as <strong>the</strong> spatial frequency response<br />

<strong>of</strong> an imaging system. It is <strong>the</strong> contrast <strong>of</strong> structures in<br />

Fig. 3.17: VIS microscope image (top, left) and <strong>the</strong>rmogram (bottom, left) <strong>of</strong> a line with a<br />

width <strong>of</strong> 34 μm on a chromium mask. Raw signal pr<strong>of</strong>ile <strong>of</strong> <strong>the</strong> line measured in <strong>the</strong> <strong>the</strong>rmogram<br />

(right) using <strong>the</strong> SC6000 camera.<br />

Forschungsbericht <strong>Research</strong> Report 2007 – 2010 83

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