Nano-optical concept design for light management

Efficient light management in optoelectronic devices requires nanosystems where high optical qualities coincide with suitable device integration. The requirement of chemical and electrical passivation for integrating nanostrutures in e.g. thin film solar cells points towards the use of insulating and stable dielectric material, which however has to provide high scattering and near-fields as well. We investigate metal@dielectric core-shell nanoparticles and dielectric nanorods. Whereas core-shell nanoparticles can be simulated using Mie theory, nanorods of finite length are studied with the finite element method. We reveal that a metallic core within a thin dielectric shell can help to enhance scattering and near-field cross sections compared to a bare dielectric nanoparticle of the same radius. A dielectric nanorod has the benefit over a dielectric nanosphere in that it can generate much higher scattering cross sections and also give rise to a high near-field enhancement along its whole length. Electrical benefits of e.g. Ag@oxide nanoparticles in thin-film solar cells and ZnO nanorods in hybrid devices lie in reduction of recombination centers or close contact of the nanorod material with the surrounding organics, respectively. The optical benefit of dielectric shell material and elongated dielectric nanostructures is highlighted in this paper.

[1]  M. Povinelli,et al.  Optical absorption enhancement in silicon nanowire arrays with a large lattice constant for photovoltaic applications. , 2009, Optics express.

[2]  I. Lauermann,et al.  Integration of plasmonic Ag nanoparticles as a back reflector in ultra-thin Cu(In,Ga)Se 2 solar cells , 2015 .

[3]  Martina Schmid,et al.  Plasmonic and photonic scattering and near fields of nanoparticles , 2014, Nanoscale Research Letters.

[4]  Richard K. Chang,et al.  Local fields at the surface of noble-metal microspheres , 1981 .

[5]  Stefan A. Maier,et al.  Low-loss fiber accessible plasmon waveguide for planar energy guiding and sensing , 2004 .

[6]  Xiang Zhang,et al.  Heterojunction silicon microwire solar cells. , 2012, Nano letters.

[7]  Electric field enhancements around the nanorod on the base layer. , 2011, Optics express.

[8]  E. Palik Handbook of Optical Constants of Solids , 1997 .

[9]  Carsten Rockstuhl,et al.  Plasmonic nanowire antennas: experiment, simulation, and theory. , 2010, Nano letters.

[10]  Craig F. Bohren,et al.  How can a particle absorb more than the light incident on it , 1983 .

[11]  Light Extraction from Plasmonic Particles with Dielectric Shells and Overcoatings , 2013 .

[12]  C. Lévy‐Clément,et al.  ZnO nanowire arrays: Optical scattering and sensitization to solar light , 2008 .

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

[14]  M. Lux‐Steiner,et al.  Hybrid solar cells with ZnO-nanorods and dry processed small molecule absorber , 2014 .

[15]  M. Schmid,et al.  Influence of substrate and its temperature on the optical constants of CuIn1−xGaxSe2 thin films , 2014 .

[16]  Laura M. Lechuga,et al.  Improved Biosensing Capability with Novel Suspended Nanodisks , 2011 .

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

[18]  J. Hafner,et al.  Localized surface plasmon resonance sensors. , 2011, Chemical reviews.

[19]  E. Yablonovitch Photonic crystals: semiconductors of light. , 2001, Scientific American.

[20]  H. Long,et al.  Tunable plasmon modes in single silver nanowire optical antennas characterized by far-field microscope polarization spectroscopy. , 2014, Nanoscale.