enhanced light trapping in thin-film solar cells by a directionally selective filter
DESCRIPTION
Enhanced light trapping in thin-film solar cells by a directionally selective filter 21 June 2010 / Vol. 18, No. 102 / OPTICS EXPRESS Carolin Ulbrich, 1,* Marius Peters, 2 Benedikt Bläsi, 2 Thomas Kirchartz, 1 Andreas Gerber, 1 and Uwe Rau 1 - PowerPoint PPT PresentationTRANSCRIPT
Enhanced light trapping in thin-film solar cells by a directionally selective filter
21 June 2010 / Vol. 18, No. 102 / OPTICS EXPRESS
Carolin Ulbrich,1,* Marius Peters,2 Benedikt Bläsi,2
Thomas Kirchartz,1 Andreas Gerber,1and Uwe Rau1
1IEF5 - Photovoltaik, Forschungszentrum Jülich, 52425Jülich, Germany 2Fraunhofer-Institut für Solare Energiesysteme,Heidenhofstraße 2, 79110 Freiburg, Germany
Advisor : H.C. Kuo / C.C. Lin
Student : H.W. Han
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Outline
Introduction
Experiment
Result
Conclusions
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Introduction
enhancement of the optical path length improving the performance of devices reducing material consumption
optical path length
with threshold value θth
this paper compare the reflection and the external quantum efficiency before and after filter deposition
wnkwwopt24
)(sin/4 22thopt wnkww
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Experiment
Bragg-like filter 73 alternating layers of
SiO2 and Ta2O5
total thickness of 5.5 µm
threshold wavelength λth
Superstrate textured SnO2:F on
AsahiU glass etched ZnO:Al on Corning
glass
Absorber layer thickness 175 nm ~ 410 nm
])(sin)()(sin2)([ 221
20
20
22 ndth
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Result (1/3)
Thickness : 322 nm ; Corning glass with etched ZnO:Al 650nm < λ < 770nm due to the directional selectivity of the filter
suppressing re-emission of non-absorbed light 350nm < λ < 650nm due to the antireflective properties of the filter short-circuit current densities Jsc : 13.40 mAcm −2 13.66 mAcm −2
- 40%
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Result (2/3)
κr represents a factor quantifying the additional light path
prolongation in the device. The large difference between the improvement factor κEQE
and κr is due to parasitic absorption in the TCO and at the back contact.
AsahiU
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Result (3/3)
the external quantum efficiency EQEfi of a 414nm thick
a-Si:H solar cell (prepared on Corning glass) The dashed line is calculated from Eq. using λ0 = 767nm
and λ1 = 600nm.)(sin)()(sin2)( 22
120
20
22 ndth
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Conclusions
a directional selective filter can improve light trapping in solar cell and enhance the overall short-circuit current density
For a-Si:H thin film solar cells the improvement depends on the texture of the front TCO and the thickness of the active absorber layer.
A maximum improvement of ΔJsc = 0.26mAcm −2
textured ZnO and an absorber thickness of 322 nm 0.06 mAcm−2 due to the antireflective effect of the filter 0.20 mAcm−2 due to its directional selectivity
limited by parasitic absorption
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Thanks for your attention!!