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

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106 CHAPTER 5<br />

a lot <strong>of</strong> space and diminishes the pixel’s fill factor to only 2.2%. In spite <strong>of</strong> the lower<br />

conversion gain the 2-side readout version is the preferable realization <strong>of</strong> both 4-tap<br />

pixels, because it <strong>of</strong>fers a three times higher fill factor (6.6%) and has a reduced<br />

demand on a highly efficient CCD charge transport. This is because the<br />

photoelectrons only have to pass three CCD gates from their generation site, the<br />

photogate, to the detection diffusion. The influences <strong>of</strong> the unconventionally shaped<br />

CCD gates <strong>of</strong> both realization versions have to be investigated thoroughly.<br />

The array-friendlier aspect ratio <strong>of</strong> 1:2 (1:1 respectively for the wheel-shaped<br />

version) and the short transport paths <strong>of</strong> the photoelectrons in the demodulation<br />

process are the major advantages <strong>of</strong> this 4-tap device compared to the multitap-<br />

CCD. However, it is not possible to realize more than four storage sites <strong>with</strong> this<br />

pixel architecture <strong>with</strong>out drastically enlarging the photogate. The photogate, on the<br />

other hand, should be as small as possible for a fast and efficient charge<br />

separation. This appeared to be a problem in the first implementation <strong>of</strong> this<br />

technique [SP1], where, due to an over-dimensioned size <strong>of</strong> the photogate<br />

compared to the relatively narrow transfer gates, an inhomogeneous sensitivity <strong>of</strong><br />

the single sampling points could be measured. By the modified, highly symmetrical<br />

pixel layouts shown in Figure 5.3 this problem <strong>of</strong> inhomogeneities between the<br />

sampling points was partly overcome, at least for low sampling frequencies.

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