Solar glass back electrode layer
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Back electrode formation for poly-Si thin film solar cells on glass
Abstract Various conductive materials (Al, Mo and TiN) were deposited onto glass substrates to evaluate whether poly-Si seed layers can be formed on such substrates by
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Dielectric Bragg Reflector as Back Electrode
A remarkable average visible transparency (AVT) of ≈52% is achieved for a semi-transparent organic solar cell. Using a dielectric Bragg reflector as infrared reflecting back electrode, the optimized
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Infrared-reflective ultrathin-metal-film-based transparent electrode
In this work we study in-depth the antireflection and filtering properties of ultrathin-metal-film-based transparent electrodes (MTEs) integrated in thin-film solar cells.
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Fabrication of anode and cathode layers for back-contact solar
Abstract The concept of back-contact device architecture for perovskite solar cells (PSCs) is a promising alternative to PSCs with the traditional sandwich-type device
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Ternary semitransparent organic solar cells with a laminated top electrode
Abstract Tinted and colour-neutral semitransparent organic photovoltaic elements are of interest for building-integrated applications in windows, on glass roofs or on facades. We demonstrate
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Effect of Glass-Coated Al Paste on Back-Surface Field
EFFECT OF GLASS-COATED Al PASTE ON BACK-SURFACE FIELD FORMATION IN Si SOLAR CELLS In this study, glass frit was coated uniformly on the surface
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Effect of back electrode composition on Copper Indium
Engineering a back electrode is one of the key factors in generating a high performance Copper Indium Gallium Selenide (CIGS) solar cell. For traditional CIGS films
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Dielectric Bragg Reflector as Back Electrode for
A remarkable average visible transparency (AVT) of ≈52% is achieved for a semi-transparent organic solar cell. Using a dielectric Bragg reflector as infrared reflecting back
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Sputtering of Molybdenum as a Promising Back Electrode
Sb 2 S 3 is rapidly developed as light absorber material for solar cells due to its excellent photoelectric properties. However, the use of the organic hole transport layer of Spiro
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Nickel-Doped Graphite and Fusible Alloy Bilayer Back
In summary, we present an innovative bilayer structured back electrode composed of a layer of low-cost Ni-doped natural graphite for interfacial charge extraction and a fusible
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Bifacial CdS/CdTe thin-film solar cells using a transparent
A hybrid silver nanowires (AgNWs)/indium tin oxide (ITO) contact was used as a transparent back-electrode to fabricate a bifacial CdS/CdTe thin-film solar cell. The
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What is a bilayer structured back electrode?
In summary, we present an innovative bilayer structured back electrode composed of a layer of low-cost Ni-doped natural graphite for interfacial charge extraction and a fusible metal alloy layer for charge transport.
Can a bilayer back electrode be deposited in a vacuum-free approach?
Here, we report a bilayer back electrode configuration consisting of an Ni-doped natural graphite layer with a fusible Bi-In alloy. This back electrode can be deposited in a vacuum-free approach and enables PSCs with a power conversion eficiency of 21.0%.
Can gold be used as a back metal electrode?
At present, gold is commonly used as the back metal electrode in state-of-the-art n-i-p structured PSCs due to its compatible work function, chemical inertness, and high conductivity. However, the high cost of gold and the expensive and time-consuming vacuum-based thin-film coating facilities may impede large-scale industrialization of PSCs.
How thick is a thin film solar cell?
Since the undercoat is not in direct contact with the solar cell, film’s thicknesses varied in the range 10–200 nm. For the cell, we consider high-efficiency, thin-film solar cells, namely perovskite solar cells (PSCs), with optimal band-gap (~ 1.4–1.5 eV) and PCE > 20%.
