Photonics and Lasers

Chapter 14.6 - Detector Circuits

14-6. DETECTOR CIRCUITS

 

So far, we have considered only the simple detector circuits shown in Fig. 14-2, in which the output is taken as the voltage across the series load resistor RL. Here, we consider two types of detector circuits that provide not only the proper bias for the diode, but also a degree of amplification.

 

14_06_Photonics_and_Lasers-2.jpg

Figure 14-17 The specific detectivity parameter D* for some respresentative photodetector materials. The maximum possible D* decreases at longer wavelength because the dark current is higher for narrower-band-gap semiconductors.

 

High-Impedance Amplifier

Figure 14-18 shows one scheme for amplifying the signal in a photodiode circuit. This is basically the same as the circuits of Fig. 14-2, except that an additional amplification stage has been added with an FET (field effect transistor). The voltage generated across the load resistor is applied between the gate (G) and source (S) of the FET, and this results in an amplified output voltage between the source and drain (D). For the best possible SNR, the photodiode can be operated in the photovoltaic mode, where VB = 0 and there is no dark current. The signal output will be proportional to RL(below saturation), so higher RLis best for detecting very small signals. This circuit is a good choice when the best possible SNR is desired.

If time response is important, however, this is not the best circuit to use. The large load resistance, in combination with the diode capacitance Cdiode, gives a 3 dB electrical bandwidth:

14_06_Photonics_and_Lasers-1.jpg

This circuit, then, suffers from the same sensitivity/time response trade-off that we discussed earlier.

Transimpedance Amplifier

When response time is important, a better choice for detector circuit is the one shown in Fig. 14-19. This circuit uses an operational amplifier (op-amp) to convert the photocur-rent i directly into an output voltage, hence the term transimpedance amplifier. The op-amp has the property that the two input terminals are held at nearly the same potential (virtual ground), while at the same time very little current is allowed to flow into or out of either terminal. For the purpose of biasing the photodiode, then, the op-amp input acts like a short circuit (RL = 0), which keeps the diode below saturation for any level of light input. Any photocurrent must flow not through the input terminals of the op-amp, but

 

14_06_Photonics_and_Lasers-3.jpg

Figure 14-18 High-impedance FET amplifier circuit for the photodiode.

 

rather through the feedback resistor RF, which is connected between the input and output of the op-amp. The output voltage is then equal to the voltage across this feedback resistor, Vout= i RF, since both input terminals of the op-amp are at ground potential. The circuit acts as if RL = RFin terms of the output voltage, but it acts as if RL= 0 in terms of biasing the photodiode. This gives the best possible linearity and dynamic range for the photodiode, and the output voltage is in fact limited only by the maximum output voltage of the op-amp (typically ~ 10 V).

A further advantage of the transimpedance amplifier is seen in the time response. Since the diode voltage is held essentially constant, the capacitance of the diode's p-n junction no longer limits the time response. Instead, it is the feedback capacitance CF characteristic of the op-amp that matters, and the bandwidth becomes

14_06_Photonics_and_Lasers-4.jpg

Since CFcan be much smaller than Cdiode, the transimpedance amplifier can have a much higher bandwidth for the same sensitivity (RF = RL). This type of detector circuit is the preferred one in many situations, because of the advantages of high speed and large dynamic range. The only drawback is in obtaining the best possible SNR for weak signals, in which case a photodiode in the photovoltaic mode followed by a high-impedance amplifier is the best choice.

 

14_06_Photonics_and_Lasers-5.jpg

Figure 14-19 Transimpedance amplifier circuit for the photodiode.

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