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w w w. p v - te ch . o rg
Cell
Processing
using the method of Aberle et al. [2]. The
experimentally determined full-area
quantum efficiencies are then active-area
corrected as shown in Fig. 2 (the correction
is for reflection from
the metallized areas as
schematically depicted in Fig. 3).
In the following, the corresponding
measurement results for a standard Al-BSF
solar cell fabricated at SERIS (schematic
shown in Fig. 6) are given.
Current losses
Quantification
of the losses in the
maximum power point current density
(
J
mpp
) is carried out by applying a bottom-
up loss analysis [1] that quantifies the seven
most important
current loss mechanisms,
i.e. (1) front metal grid shading; (2) front-
surface reflectance in the active area; (3)
front-surface escape; (4)
shunt resistance; (5)
non-perfect active-area quantum efficiency;
(6) forward bias current at the maximum
power point (‘diode recombination’); and
(7) photon absorption within the front-side
dielectric passivation/anti-reflective (AR)
layer (i.e.
silicon nitride SiN
x
).
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