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CMOS Optical Preamplifier Design Using Graphical Circuit Analysis

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E e<br />

+<br />

-<br />

V bias<br />

2.1 Photodetectors 11<br />

The main photocurrent, , is generated through the creation of electron-hole<br />

pairs when photons from the incident light penetrate the diode. The sensitivity of the<br />

photodetector is a function of the wavelength, and so to maximize power efficiency,<br />

the emission wavelength of the optical source should be spectrally matched to the<br />

photodiode. Silicon photodiodes, which are commonly used in low-cost applica-<br />

tions, have a peak spectral efficiency in the near infrared region. Figure 2.2 shows<br />

the normalized spectral sensitivity of a typical silicon photodiode 1 , and shows how<br />

it is spectrally matched to GaAs LEDs (e.g. Temic TSHF5400).<br />

Relative sensitivity (%)<br />

1. Data taken from Temic’s BPV22NF photodiode.<br />

i<br />

s<br />

Figure 2.1 Small-signal equivalent circuit model of photodiode.<br />

100<br />

90<br />

80 80<br />

Relative sensitivity (%)<br />

70<br />

60 60<br />

50<br />

40 40<br />

30<br />

20 20<br />

10<br />

0<br />

GaP:N<br />

LED<br />

i s<br />

GaAsP<br />

LED<br />

GaAs<br />

LED<br />

2<br />

I n<br />

GaAs:Si<br />

LED<br />

C d<br />

Si<br />

photodiode<br />

R s<br />

+<br />

V bias<br />

0<br />

300 400 300 Ultra-<br />

500 600<br />

Visible<br />

700 800 900 1000<br />

Near<br />

1100 1200 1300<br />

1400 1500<br />

violet<br />

light<br />

infrared<br />

Wavelength (nm)<br />

Ultraviolet<br />

Visible<br />

Near<br />

infrared<br />

Wavelength(nm)<br />

Figure 2.2 Relative spectral sensitivity of Temic BPV22NF silicon photodiode and<br />

emission peaks of several types of LEDs.<br />

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