
+V-V
+I
-I
PC Load Line PV Load Line
L=1
L=2
L=4
L=3
Figure 2
L= Illumination
I= Current generated from the photodiode
Load Line = I/RLoad
“Improving the Quality of Life through the Power in Light”
…photovoltaic & photoconductive… …features…
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When a photodiode is operated in a photovoltaic mode, the
photodiode is unbiased. During the time that the photodiode operates
with a reverse bias voltage, the operating mode is considered
photoconductive. Figure 2 shows a typical I-V curve for a silicon
photodiode. This graph indicates the increase in relative current to
the increase in illumination at V=0 (short circuit current). The
illumination curves are linear to input light intensity until the
photodiode becomes forward biased, at this point the generated
current starts to flow through the diode. Photodiode open circuit
voltage is where I=0 on the illumination curve (diode is forward
biased) and varies as the logarithm of the illumination level. Both
the photovoltaic load (PV) and the photoconductive (PC) load lines
are indicated in figure 2 as well. As shown, the PV load line
indicates a linear current vs. illumination is generated for
illuminations L=1 and L=2; while the PV load line indicates a non-
linear current vs. illumination for L=3 and L=4 as the diode becomes
forward biased. The PC load line will maintain a linear current vs.
illumination for all illumination levels.
Figures 3a and 3b are typical for photovoltaic operation. Photovoltaic
applications are designed for low noise (reduced dark currents) and the
frequency response of figure 3a will be dependant on load resistance and
the shunting impedance of the photodiode junction capacitance
[1/(2πFC)]. The circuit shown in figure 3b illustrates a transimpedance
amplifier. This amplifier will clamp the photodiode voltage bias to zero
volts. The resultant effective impedance seen by the junction capacitance
will be very low yielding excellent frequency response.
Figures 4a and 4b illustrate circuits typical for photoconductive
applications. A photoconductive mode of operation will enhance the
photodiode speed requirements as the junction capacitance is reduced with
increase in reverse bias. The reverse bias will generate a dark current
proportional to the bias voltage and should be evaluated for the particular
application. The circuits in Figure 4 are similar to the Figure 3 above,
except the photodiodes are operated with a reverse bias.
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. offers two high quality, state of the
art, photodiode constructions: Photovoltaic for (PV)
application and Photoconductive for (PC) applications. Due
to the high quality of our design the two series can be used in
both photovoltaic and photoconductive modes.
¾ The PV series is slightly lower in dark current while
designed to minimize the internal series resistance to
enhance the linearity of illumination response levels well
into the forward biased operation point.
¾ The PC series is designed to provide a low junction
capacitance while providing excellent dark current
parameters. The PC series will also provide improved far-
red spectral response.
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¾ Linearity Over a Wide Dynamic
Range
¾ Broad Spectral Response
¾ Excellent Responsivity
PC
Low Capacitance
Low Dark Current
PV
High Shunt Resistance
Low Noise