Programm Photovoltaik Ausgabe 2009 ... - Bundesamt für Energie BFE
Programm Photovoltaik Ausgabe 2009 ... - Bundesamt für Energie BFE Programm Photovoltaik Ausgabe 2009 ... - Bundesamt für Energie BFE
3/16 The project’s goals are, hence, to be achieved by introducing innovation and optimisation in four majors areas: � Layers with new or better properties (e.g. new materials with higher transparency) � Improved processes (more stable, faster processes, yielding higher quality layers) � Increased device and module efficiency � Enhanced cells and modules reliability. Work performed and results achieved 1. Materials 1.1 Development of advanced SiOx based intermediate reflectors [Bue08]. The material properties of doped silicon oxide intermediate reflectors deposited in situ with plasma enhanced chemical vapor deposition systems has been investigated. The challenge in the development of these layers is to lower the refractive index without compromising the electrically conductive properties. Intermediate reflectors are used in micromorph tandem cells to increase the current density in thin top amorphous cells. Low refractive indices are therefore desirable because the reflectivity of the layer depends on the index step between silicon oxide and silicon. However, lower refractive indexes are typically associated with increasingly more insulating layers which can block the current flow between top and bottom cell. In order to better understand the trade-off between optical and electrical requirements of the silicon oxide intermediate reflector, the structure of the layers was analyzed with bright field TEM images. In the images of Figure 2, silicon nanocrystals embedded in an amorphous silicon oxide matrix can be seen. For increasing H2 dilution the silicon nanocrystals are reduced in number and in size. Accordingly, the conductivity of the layers decreases (not shown). This correlation suggests that the conductive properties of doped silicon oxide intermediate reflectors are associated with the presence of densely distributed and large silicon nanocrystals. These nanocrystals most likely are the conductive channels through which the current flows. Deposition parameters were varied in order to find a conductive layer with the lowest possible refractive index. Fig.3 shows the refractive index of intermediate reflective layers as a function of CO2/SiH4 and H2/SiH4 gas ratios. For both series, the refractive index decreases with increasing CO2/SiH4 gas ratio. As a result of this process optimization a conductive silicon oxide layer with refractive index n = 1.71 has been developed and used in micromorph tandem cells. Fig.2: TEM top-view images of ~ 100 nm thick nc-SiOx layers deposited at different dilutions Fig.3: Refractive index of silicon oxide layers with various preparation conditions 33/290 New processes and device structures for the fabrication of high efficiency thin film silicon photovoltaic modules, C. Ballif, University of Neuchâtel
1.2. Comparison of ZnO and SiOx intermediate reflectors on various TCO’s [Dom08,Dom08b] Silicon oxide intermediate reflectors were inserted at the recombination junction of micromorph tandem cells in p-i-n configuration deposited by very-high frequency plasma enhanced chemical vapour deposition (VHF-PECVD). All the layers were deposited in a laboratory scale dual chamber deposition system. For comparison, intermediate reflectors made out of ZnO were also processed. In [Dom08, Dom08B], the influence of the nature of the intermediate reflector (SiOx or ZnO) on the current matching and cell performance was investigated in detail. It was shown (Fig.4a) that both reflectors acts very similarly, whereas and increased grain size could lead up to 1.8 mA/cm2 in full micromorph devices. The effectiveness of the intermediate reflector was shown to be higher for small grain TCO (Fig.4b). a) b) Fig.4: a) EQEs of micromorph cells with 150 nm thick SOIR layers deposited on type-A (small size) and type-C (large size) front ZnO. b) current in top and bottom cells for various roughness of the front TCO. 1.3 LP-CVD Transparent conducting zinc oxide (ZnO) and TCO’s [Ste08] The in-house LPCVD ZnO developed at IMT is particularly well suited as electrodes in thin film silicon amorphous and micromorph solar cells because, in addition to good transparency and conductivity properties, it possesses an as-grown rough surface texture that efficiently scatters the light. Commercially available solar modules, in which LPCVD ZnO is already used as electrodes, are submitted to standard stability test like damp heat exposure. ZnO is known to have its electrical conductivity degraded by a humid environment. Even if encapsulated modules using LPCVD ZnO:B layers have been shown by Oerlikon Solar [Kro06] to successfully pass the standard damp heat test (exposure to 85% humidity at 85°C during 1000 hours), it is important to understand the stability behavior of LPCVD ZnO:B films in a humid environment as these properties will dictate some of the requirements on the encapsulation. a) b) Fig.5: a) Optical and Hall mobility of a 2 µm thick standard doped LPCVD ZnO:B film in function of the damp heat exposure (40°C, 100% humidity) time b) Carrier concentration detected optically and measured by the hall effect [Stei08] 34/290 New processes and device structures for the fabrication of high efficiency thin film silicon photovoltaic modules, C. Ballif, University of Neuchâtel 4/16
- Page 1: Forschung, April 2009 Programm Phot
- Page 4 and 5: Programm Photovoltaik Ausgabe 2009
- Page 6 and 7: B. Ruhstaller, R. Häusermann, N. A
- Page 8 and 9: PROGRAMM PHOTOVOLTAIK Eidgenössisc
- Page 10 and 11: 1. Programmschwerpunkte und anvisie
- Page 12 and 13: Eine zweite Kategorie von Projekten
- Page 14 and 15: Im Integrierten EU-Projekt ATHLET [
- Page 16 and 17: Figur 3: Prototyp eines monolithisc
- Page 18 and 19: SOLARMODULE UND GEBÄUDEINTEGRATION
- Page 20 and 21: BEGLEITENDE THEMEN Das PSI beteilig
- Page 22 and 23: Programme abgeschlossen. Die erste
- Page 24 and 25: Messkampagnen - Messkampagne Wittig
- Page 26 and 27: zielführend eingesetzt werden. Das
- Page 28 and 29: [43] P. Renaud, L. Perret, (pierre.
- Page 30: 11. Verwendete Abkürzungen (inkl.
- Page 33 and 34: D. Güttler, S. Bücheler, S. Seyrl
- Page 35: Goals of the project The global pro
- Page 39 and 40: 2. Processes 2.1. Microcrystalline
- Page 41 and 42: 3.2. Amorphous/amorphous silicon ta
- Page 43 and 44: Fig.14: TEM cross section microcrys
- Page 45 and 46: EQE 1.0 0.8 0.6 0.4 0.2 12.4 11.7 1
- Page 47 and 48: 4.7 Summary and perspectives for wo
- Page 49 and 50: Acknowledgements We thank all the P
- Page 51 and 52: Goals of the project The goals of t
- Page 54 and 55: Eidgenössisches Departement für U
- Page 56: 3/3 on the front side. All the laye
- Page 59 and 60: Introduction / Project Goals Prior
- Page 62 and 63: Eidgenössisches Departement für U
- Page 64 and 65: 3/4 Effective light trapping scheme
- Page 66 and 67: Département fédéral de l’envir
- Page 68 and 69: 3/6 The Athlet consortium comprises
- Page 70 and 71: 5/6 Large area thin-film silicon ce
- Page 72 and 73: Eidgenössisches Departement für U
- Page 74 and 75: 3/4 Der verbesserte Lichteinfang is
- Page 76 and 77: Eidgenössisches Departement für U
- Page 78 and 79: 3/5 Results Microstructure characte
- Page 80: 5/5 Mechanical testing: The mechani
- Page 83 and 84: Introduction / Project goals The fo
- Page 85 and 86: Optimization of CdS chemical bath d
3/16<br />
The project’s goals are, hence, to be achieved by introducing innovation and optimisation in four majors<br />
areas:<br />
� Layers with new or better properties (e.g. new materials with higher transparency)<br />
� Improved processes (more stable, faster processes, yielding higher quality layers)<br />
� Increased device and module efficiency<br />
� Enhanced cells and modules reliability.<br />
Work performed and results achieved<br />
1. Materials<br />
1.1 Development of advanced SiOx based intermediate reflectors [Bue08].<br />
The material properties of doped silicon oxide intermediate reflectors deposited in situ with plasma<br />
enhanced chemical vapor deposition systems has been investigated. The challenge in the development<br />
of these layers is to lower the refractive index without compromising the electrically conductive<br />
properties. Intermediate reflectors are used in micromorph tandem cells to increase the current density<br />
in thin top amorphous cells. Low refractive indices are therefore desirable because the reflectivity of<br />
the layer depends on the index step between silicon oxide and silicon. However, lower refractive indexes<br />
are typically associated with increasingly more insulating layers which can block the current flow<br />
between top and bottom cell. In order to better understand the trade-off between optical and electrical<br />
requirements of the silicon oxide intermediate reflector, the structure of the layers was analyzed with<br />
bright field TEM images. In the images of Figure 2, silicon nanocrystals embedded in an amorphous<br />
silicon oxide matrix can be seen. For increasing H2 dilution the silicon nanocrystals are reduced in<br />
number and in size. Accordingly, the conductivity of the layers decreases (not shown). This correlation<br />
suggests that the conductive properties of doped silicon oxide intermediate reflectors are associated<br />
with the presence of densely distributed and large silicon nanocrystals. These nanocrystals most likely<br />
are the conductive channels through which the current flows.<br />
Deposition parameters were varied in order to find a conductive layer with the lowest possible refractive<br />
index. Fig.3 shows the refractive index of intermediate reflective layers as a function of CO2/SiH4<br />
and H2/SiH4 gas ratios. For both series, the refractive index decreases with increasing CO2/SiH4 gas<br />
ratio. As a result of this process optimization a conductive silicon oxide layer with refractive index n =<br />
1.71 has been developed and used in micromorph tandem cells.<br />
Fig.2: TEM top-view images of ~ 100 nm thick nc-SiOx layers deposited at different dilutions<br />
Fig.3: Refractive index of silicon oxide layers with various preparation conditions<br />
33/290<br />
New processes and device structures for the fabrication of high efficiency thin film silicon photovoltaic modules, C. Ballif, University of Neuchâtel