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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SOLID-STATE IMAGE SENSING 53<br />
immediately separated and captured, extends up to d0 + wsc, where d0 is the<br />
position <strong>of</strong> the pn-junction.<br />
VDD VSS V SS<br />
V DD<br />
n+ diode<br />
p - (substrate) n - (n-well) p + n +<br />
V SS V DD<br />
n-well diode<br />
V SS V DD<br />
Diffusion Depth <strong>of</strong><br />
junction<br />
Doping<br />
concentration<br />
n+ diffusion 200 nm 2⋅10 20 cm -3<br />
n-well 3700 nm 5⋅10 16 cm -3<br />
p-substrate 5⋅10 15 cm -3<br />
Photodiode wsc for Vr=5 V Active depth<br />
(wsc + junct.<br />
depth)<br />
n+ diode 1.2 µm 1.4 µm<br />
n-well diode 1.2 µm 4.9 µm<br />
Figure 3.2 Realizations <strong>of</strong> photodiodes in a CMOS process. The tables give<br />
typical values <strong>of</strong> doping concentration and depth <strong>of</strong> the diffusion<br />
regions for 0.5µm CMOS process. Also the width <strong>of</strong> the space<br />
charge region is calculated.<br />
Penetration depth <strong>of</strong> light<br />
The absorption <strong>of</strong> photons entering the semiconductor material is a statistical<br />
process. The sites <strong>of</strong> photon-absorption are statistically distributed <strong>with</strong> an<br />
exponential dependence <strong>of</strong> <strong>distance</strong> from the semiconductor surface and<br />
1<br />
wavelength <strong>of</strong> the incoming light. The <strong>distance</strong> where an amount <strong>of</strong> = 37%<br />
<strong>of</strong> the<br />
e<br />
total photon flux Φ(x) is already absorbed is called the penetration depth. That is<br />
the inverse <strong>of</strong> the absorption constant α [Sze].<br />
⎛ −x<br />
⎞<br />
⎜<br />
⎟<br />
( −α⋅x<br />
Φ = Φ ⋅<br />
)<br />
= Φ ⋅ ⎝ penetration<br />
depth<br />
( x)<br />
⎠<br />
o e<br />
o e<br />
Equation 3.2<br />
Figure 3.3 illustrates the exponential attenuation <strong>of</strong> the photon flux in silicon.