“…Among them, the 1-Diode/2-Resistor equivalent circuit model was selected, see Figure 6 B. It is basically composed of a current source connected in parallel with a diode, together with a shunt resistance R sh , and a series resistance R s [ 16 , 17 , 18 , 19 ]. Using the Shockley model for the diode, the output current, I , and the output voltage, V , at the terminals of the photodiode are related implicitly by the following equation: where I pv is the photovoltaic current, I 0 is the reverse saturation current of the diode, a is the ideality factor, R sh is the shunt resistor, R s is the series resistor, and V T is the thermal voltage of the diode, which is expressed in terms of the temperature, T , the Boltzmann’s constant, κ , and the electron charge q as: …”