A. Dhingra et A. Rothwarf, COMPUTER-SIMULATION AND MODELING OF GRADED BANDGAP CUINSE2 CDS BASED SOLAR-CELLS/, I.E.E.E. transactions on electron devices, 43(4), 1996, pp. 613-621
This paper proposes graded bandgap absorber material, Cu1-xAgxIn1-y-zG
ayAlxSe2(1-u-w)S2uTe2w (CIS) multinary system, to improve the low ope
n-circuit voltage (V-OC) seen in CuInSe2/CdS solar cells, without sacr
ificing the short-circuit current density (J(sc)). It also proposes a
p-i-n model for the CuInSe2/CdS solar cell, where the intrinsic region
is the graded bandgap CIS. Reflecting surfaces are provided at the p
- i and n - i interfaces to trap the light in the narrow intrinsic re
gion for maximum generation of electron and hole pairs (EHP's). This o
ptical confinement results in a 25-40% increase in the number of photo
ns absorbed. An extensive numerical simulator was developed, which pro
vides a 1-D self-consistent solution for Poisson's equation and the tw
o continuity equations for electrons and holes. This simulator was use
d to generate J - V curves to delineate the effect of different gradin
g profiles on cell performance. The effects of a uniform bandgap, norm
al grading, reverse grading, and a low bandgap notch have been conside
red. Having established the inherent advantages to these grading profi
les an optimal doubly graded structure is proposed with grading betwee
n 1.5 eV and 1.3 eV regions which has V-oc = 0.86 V, eta = 17.9%, FF =
0.79 and J(sc) = 26.3 mA/cm(2) compared to 0.84 V, 14.9%, 0.76, and 2
3.3 mA/cm(2), respectively, for the highest efficiency 1.4-eV uniform
bandgap cell. Replacing the thick CdS(2.42ev) layer assumed in our sim
ulations with a aide gap semiconductor such as ZnO(3.35ev) increases a
ll current densities by about 5 mA/cm(2), and increases the optimal ca
lculated efficiency from 17.9% to roughly 21% for a doubly graded stru
cture with a thickness of 1 mu m and bandgaps ranging from 1.3 eV to 1
.5 eV.