Literature DB >> 22805108

Polycrystalline silicon thin-film solar cells with plasmonic-enhanced light-trapping.

Sergey Varlamov1, Jing Rao, Thomas Soderstrom.   

Abstract

One of major approaches to cheaper solar cells is reducing the amount of semiconductor material used for their fabrication and making cells thinner. To compensate for lower light absorption such physically thin devices have to incorporate light-trapping which increases their optical thickness. Light scattering by textured surfaces is a common technique but it cannot be universally applied to all solar cell technologies. Some cells, for example those made of evaporated silicon, are planar as produced and they require an alternative light-trapping means suitable for planar devices. Metal nanoparticles formed on planar silicon cell surface and capable of light scattering due to surface plasmon resonance is an effective approach. The paper presents a fabrication procedure of evaporated polycrystalline silicon solar cells with plasmonic light-trapping and demonstrates how the cell quantum efficiency improves due to presence of metal nanoparticles. To fabricate the cells a film consisting of alternative boron and phosphorous doped silicon layers is deposited on glass substrate by electron beam evaporation. An Initially amorphous film is crystallised and electronic defects are mitigated by annealing and hydrogen passivation. Metal grid contacts are applied to the layers of opposite polarity to extract electricity generated by the cell. Typically, such a ~2 μm thick cell has a short-circuit current density (Jsc) of 14-16 mA/cm(2), which can be increased up to 17-18 mA/cm(2) (~25% higher) after application of a simple diffuse back reflector made of a white paint. To implement plasmonic light-trapping a silver nanoparticle array is formed on the metallised cell silicon surface. A precursor silver film is deposited on the cell by thermal evaporation and annealed at 23°C to form silver nanoparticles. Nanoparticle size and coverage, which affect plasmonic light-scattering, can be tuned for enhanced cell performance by varying the precursor film thickness and its annealing conditions. An optimised nanoparticle array alone results in cell Jsc enhancement of about 28%, similar to the effect of the diffuse reflector. The photocurrent can be further increased by coating the nanoparticles by a low refractive index dielectric, like MgF(2;), and applying the diffused reflector. The complete plasmonic cell structure comprises the polycrystalline silicon film, a silver nanoparticle array, a layer of MgF(2;), and a diffuse reflector. The Jsc for such cell is 21-23 mA/cm(2), up to 45% higher than Jsc of the original cell without light-trapping or ~25% higher than Jsc for the cell with the diffuse reflector only.

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Year:  2012        PMID: 22805108      PMCID: PMC3471272          DOI: 10.3791/4092

Source DB:  PubMed          Journal:  J Vis Exp        ISSN: 1940-087X            Impact factor:   1.355


  2 in total

1.  Plasmonic solar cells.

Authors:  K R Catchpole; A Polman
Journal:  Opt Express       Date:  2008-12-22       Impact factor: 3.894

2.  Resonant SPP modes supported by discrete metal nanoparticles on high-index substrates.

Authors:  F J Beck; E Verhagen; S Mokkapati; A Polman; K R Catchpole
Journal:  Opt Express       Date:  2011-03-14       Impact factor: 3.894

  2 in total
  1 in total

Review 1.  Current Approach in Surface Plasmons for Thin Film and Wire Array Solar Cell Applications.

Authors:  Keya Zhou; Zhongyi Guo; Shutian Liu; Jung-Ho Lee
Journal:  Materials (Basel)       Date:  2015-07-22       Impact factor: 3.623

  1 in total

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