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    The University of New South Wales

    Development and Optimization ofLaser-Doped Solar Cells

    Ziv Hameiri

    13/6/2012

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    Contents

    Introduction

    Laser doping

    Optimization:

    Laser-Induced Defects in Laser-Doped Solar Cells

    Influence of Metallisation Methods

    Influence of Laser Power on Laser-Doped Solar Cells

    Conclusions

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    Introduction

    In order to make solar energy cost-competitive withother sources of energy (i.e. fossil fuels), reduction ofthe PV system cost is essential

    One path to reduce the cost is to reduce the raw

    material cost, by reducing the amount of silicon used fora wafer or by employing a lower quality of silicon, whichis cheaper to produce

    The second path is increasing the solar systemefficiency without significantly increasing themanufacturing cost

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    Introduction

    Solar technologies market report, NREL, 2008

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    Introduction

    However, standard industrial solar cell efficiency is in the16-18% range

    Main limitations of the high-efficiency structure:

    Very expensive

    Very long fabrication process

    small output(five different photo-lithographic processes, eight high temp.processes!)

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    Introduction

    Selective emitter

    Local back-surface-field

    Rear surface passivationAluminum back-surface-field

    Green MA. Silicon Solar Cells: Advanced Principles & Practice, 1995

    PERLStandard solar cell

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    Introduction

    The Aim:

    To develop an industrial version of the high-efficiency solar cell structure

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    IntroductionSelective Emitter SC

    Main limitation:A long high-temperature process is required to create theselective emitter.

    [2-7]

    The buried-contacts solar cell

    (UNSW)

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    Laser Doping

    Creation of selective emitter without additional hightemperature process

    1968: Fairfield and Schwuttke laser doped diode

    Laser-induced diffusion: Diffusion in the liquid phase

    Different dopant sources in gas, liquid and solid states

    Fairfield J, Schwuttke GH. Solid State Electronics1968; 11: 1175-1176

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    Laser Doping

    Dopant

    source

    Dielectriclayern++ n++ n++

    Not to scale

    p-type wafer Emitter

    Al BSF

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    Influence of Laser Power

    .

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    Influence of Laser Power

    .

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    OPTIMIZATION OF LDSE SOLAR CELLS

    LASER INDUCED DEFECTS

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    Laser-Induced Defects

    .

    Bare Samples

    SiNx Sample

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    Laser-Induced Defects

    .

    Bare Sample SiNX Sample

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    SON Sample

    Laser-Induced Defects

    .

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    Laser-Induced Defects

    Solar Cell Results:

    .

    Defect density can be reduced by adding a thin SiO2 layer

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    OPTIMIZATION OF LDSE SOLAR CELLS

    PLATING METHOD

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    Influence of Metallisation Methods

    .

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    Influence of Metallisation Methods

    .

    Dark I-V curve:

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    Influence of Metallisation Methods

    Conclusions:

    Higher p-FFs were achieved for photoplated laser-dopedsolar cells

    p-FF is almost independent of laser diode current ifphotoplating is combined with a well-optimised Ni sintering

    In this case the solar cell is not limited by shunts

    .

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    INFLUENCE OF LASER POWER

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    Influence of Laser Power on Solar cells

    Solar Cells:

    .

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    Influence of Laser Power on Solar cells

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    Conclusions

    Selective emitter solar cell structure was developed,based on laser doping

    The laser doping method offers significant control onthe junction parameters (sheet resistivity and junction

    depth) The dielectric layer and the plating method have a large

    impact on the solar cell performance

    Efficiency of 18.7% was achieved on commercial CZ

    wafers

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    Laser-Induced Defects

    .

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    The School of Photovoltaic and Renewable Energy Engineering

    THANK YOU

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    The School of Photovoltaic and Renewable Energy Engineering

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