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3D Time-of-flight distance measurement with custom - Universität ...

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134 CHAPTER 5<br />

We see that even for 10 V the saturation velocity is not yet reached. The results we<br />

presented (increase in demodulation contrast for increased PGL / PGR voltage) are<br />

reasonable because an increase in electrical field still causes an increased drift<br />

velocity and hence faster response <strong>of</strong> charge carriers to the electrical field, leading<br />

to a better demodulation contrast at high modulation frequencies.<br />

5.2.4 Influence <strong>of</strong> optical power and integration time @ 20MHz<br />

We discussed in Section 3.2 that the charge transfer efficiency <strong>of</strong> CCDs strongly<br />

depends on the number <strong>of</strong> charge carriers that are contained in the charge packet<br />

to transport (c.f. Figure 3.20). Therefore we expect the optical power, i.e. how<br />

many photoelectrons are generated (and hence have to be transported) per unit<br />

time, to have a noticeable influence on the demodulation contrast. This is<br />

investigated in the current section.<br />

In order to measure the influence <strong>of</strong> the number <strong>of</strong> generated photoelectrons per<br />

unit time on the contrast, two parameters are changed: (1) the optical power and (2)<br />

the integration times. For a good reproducibility <strong>of</strong> the <strong>measurement</strong>s we keep the<br />

output power <strong>of</strong> the LED constant and use neutral density filters (ND) to attenuate<br />

the power on the pixel. This has the advantage that the LED can be operated <strong>with</strong><br />

the same mean current (50 mA) for all <strong>measurement</strong>s. (Because <strong>of</strong> a currentdependent<br />

operating temperature, the LED changes its dynamic characteristics for<br />

different control currents). For each integration time we chose a different spot size<br />

(by adjusting the <strong>distance</strong> <strong>of</strong> the microscope’s objective to the sensor chip), the<br />

exact parameters are summarized in MCD05 in the appendix.<br />

We carry out <strong>measurement</strong>s <strong>of</strong> the demodulation contrast for 4 different optical<br />

power conditions (1) <strong>with</strong>out ND filter, (2) <strong>with</strong> 27% ND filter (3) <strong>with</strong> 8% ND filter<br />

and (4) <strong>with</strong> both intensity filters (2% attenuation). Since the total optical power and<br />

the size <strong>of</strong> the light spot are measured, we can recalculate the optical power on the<br />

light sensitive area <strong>of</strong> each pixel. The dark current is measured separately and<br />

subtracted from the measured values before calculating the demodulation contrast.<br />

These <strong>measurement</strong>s have only been performed for the surface-channel realization<br />

(SCCD); the results are shown in Figure 5.19 and Figure 5.20.

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