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 ...
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DEMODULATION PIXELS IN CMOS/CCD 101<br />
This chapter is divided into three main sections: In Section 5.1 we introduce<br />
different realizations <strong>of</strong> demodulation pixels. They have all been realized in Orbit<br />
2 µm CMOS/CCD technology, a process <strong>of</strong>fered as MPW. This process has two<br />
different polysilicon layers (poly1 and poly2) that can both be used as transistor<br />
gates. Additionally the design rules allow these poly gates to overlap over the thin<br />
gate oxide. Hence it is possible to realize CCDs <strong>with</strong> this CMOS/CCD process (c.f.<br />
Section 3.2). The realized demodulation pixels vary in operational architecture,<br />
maximum demodulation frequency and fill factor, the latter being a very important<br />
parameter for realizing highly sensitive devices. All pixels fulfill the four physical<br />
demodulation demands described above. The characteristic features <strong>of</strong> the pixels<br />
introduced are summarized in Table 5.1 and Figure 5.8.<br />
Section 5.2 then summarizes the results <strong>of</strong> a detailed characterization <strong>of</strong> the<br />
demodulation performance for the 1-tap pixel, which is the pixel-realization <strong>with</strong> the<br />
best electrooptical properties (demodulation bandwidth and optical fill factor). This<br />
pixel has been fabricated twice; (1) <strong>with</strong> surface channel (SCCD) CCD structures<br />
and (2) <strong>with</strong> buried channel (BCCD) structures, allowing a direct comparison <strong>of</strong> both<br />
CCD types. Especially we focus on the efficiency <strong>of</strong> the shutter mechanism<br />
(sampling efficiency or demodulation contrast) and its dependency on sampling<br />
frequency and wavelength. Also, we present the measured phase accuracy as a<br />
function <strong>of</strong> the optical power received in the pixel and compare these results to the<br />
theory presented in Section 4.2. The 1-tap pixel is the basis for two lock-in sensor<br />
arrays we realized, a line-sensor <strong>with</strong> 108 pixels and an image sensor <strong>with</strong> 64x25<br />
pixels. Both arrays are implemented as range cameras, which are introduced in<br />
Chapter 6.<br />
Motivated by the outstanding results presented in Section 5.2, we present a very<br />
simple and only slightly modified pixel structure in Section 5.3 that overcomes the<br />
restrictions <strong>of</strong> the 1-tap pixel (serial integration <strong>of</strong> the single sampling points) by<br />
<strong>of</strong>fering two optically identical photosites.