3D Time-of-flight distance measurement with custom - Universität ...
3D Time-of-flight distance measurement with custom - Universität ...
3D Time-of-flight distance measurement with custom - Universität ...
You also want an ePaper? Increase the reach of your titles
YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.
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.