5.4 Absorption coefficient and quantum efficiency Consider the Si pn junction photodiode shown in Figure 5.8.
Suppose that the incident optical power is P_(o). The incident number of photons per unit time is (P_(o))/(h)v. Of these, a
fraction T is transmitted. The number of photons flowing per second along the device is
(dN_(ph))/(dt)=(TP_(o))/(hv)exp(-\alpha x)
where x is measured from the illuminated surface of the semiconductor. Show that the photocurrent generated
by the photodiode is given by
I_(ph)=(e\eta _(i)TP_(o))/(hv){exp[-\alpha (l_(p)-L_(e))]-exp[-\alpha (l_(p)-L_(e)+W+L_(h))]}
where \eta _(i) is the internal quantum efficiency and the other symbols are defined in Figure 5.8. Consider two pho-
todiodes, one p^(+)n and the other pin. Their properties are listed in Table 5.7, where the photocurrent has been
calculated at 800 nm . Suppose that the incident optical power is 1\mu W, and the antireflection coating on the
semiconductor provides T~~1. Find the photocurrent I_(ph) and hence the responsivity of the two photodiodes at
900 nm and 500 nm . What is your conclusion?
TABLE 5.7 Properties of a p^(+)n and pin photodiode
Note: \eta _(i)=1,T=1 and P_(o)=1\mu W were used.