Highest Efficiency Plasmonic Polycrystalline Silicon Thin-Film Solar Cells by Optimization of Plasmonic Nanoparticle Fabrication

Excitation of surface plasmons in metallic nanoparticles is a promising method for increasing the light absorption in solar cells and hence the cell photocurrent. Comprehensive optimization of a nanoparticle fabrication process for enhanced performance of polycrystalline silicon thin-film solar cells is presented. Three factors were studied: the Ag precursor film thickness, annealing temperature and time. The thickness of the precursor film was 10, 14 and 20 nm; annealing temperature was 190, 200, 230 and 260 °C; and annealing time was varied between 20 and 95 min. Performance enhancement due to light-scattering by nanoparticles was calculated by comparing absorption, short-circuit current density and energy conversion efficiency in solar cells with and without nanoparticles formed under different process conditions. Nanoparticles formed from 14-nm-thick Ag precursor film annealed at 230 °C for 53 min result in the highest absorption enhancement in the 700–1,100 nm wavelength range, in the highest enhancement of total short-circuit current density. The highest photocurrent enhancement was 33.5 %, which was achieved by the cell with the highest absorption enhancement in the 700–1,100 nm range. The plasmonic cell efficiency of 5.32 % was achieved without a back reflector and 5.95 % with the back reflector; which is the highest reported efficiency for plasmonic thin-film solar cells.

[1]  M. Green The path to 25% silicon solar cell efficiency: History of silicon cell evolution , 2009 .

[2]  W. Tu,et al.  Hydrogenated amorphous silicon solar cell on glass substrate patterned by hexagonal nanocylinder array , 2010 .

[3]  H. Atwater,et al.  Plasmonics for improved photovoltaic devices. , 2010, Nature materials.

[4]  M. Green Solar Cells : Operating Principles, Technology and System Applications , 1981 .

[5]  Daniel Derkacs,et al.  Metal and dielectric nanoparticle scattering for improved optical absorption in photovoltaic devices , 2008 .

[6]  Albert Polman,et al.  Asymmetry in photocurrent enhancement by plasmonic nanoparticle arrays located on the front or on the rear of solar cells , 2010 .

[7]  Jongsung Park,et al.  Optimization of Dielectric-Coated Silver Nanoparticle Films for Plasmonic-Enhanced Light Trapping in Thin Film Silicon Solar Cells , 2013, Plasmonics.

[8]  Jing Chen,et al.  Efficiency enhancement of the poly-silicon solar cell using self-assembled dielectric nanoparticles , 2011 .

[9]  W. Steen Absorption and Scattering of Light by Small Particles , 1999 .

[10]  Zi Ouyang,et al.  Advances in Evaporated Solid-Phase-Crystallized Poly-Si Thin-Film Solar Cells on Glass (EVA) , 2008 .

[11]  Albert Polman,et al.  Tunable light trapping for solar cells using localized surface plasmons , 2009 .

[12]  Zi Ouyang,et al.  Nanoparticle‐enhanced light trapping in thin‐film silicon solar cells , 2011 .

[13]  M. Green,et al.  Surface plasmon enhanced silicon solar cells , 2007 .

[14]  Arnold F. McKinley,et al.  Plasmonics and nanophotonics for photovoltaics , 2011 .

[15]  Sergey Varlamov,et al.  Polycrystalline silicon thin-film solar cells with plasmonic-enhanced light-trapping. , 2012, Journal of visualized experiments : JoVE.

[16]  Martin A. Green,et al.  Harnessing plasmonics for solar cells , 2012, Nature Photonics.

[17]  Daniel Derkacs,et al.  Plasmonic nanoparticle scattering for enhanced performance of photovoltaic and photodetector devices , 2008, NanoScience + Engineering.

[18]  Albert Polman,et al.  Design principles for particle plasmon enhanced solar cells , 2008 .

[19]  Y. Akimov,et al.  Resonant and nonresonant plasmonic nanoparticle enhancement for thin-film silicon solar cells , 2010, Nanotechnology.