A brief overview of Plasmonic Nanostructure Design for Efficient Light Coupling into Solar Cells V.E. Ferry, L.A. Sweatlock, D. Pacifici, and H.A. Atwater,

Slides:



Advertisements
Similar presentations
T HIN FILM SOLAR CELLS Presented by Yao Sun. F UTURE ENERGY SOURCE Clean energy Most reasonable price for the future Available anywhere in the world 1.52*10^21.
Advertisements

Solar cells Yogesh Wakchaure.
Nanophotonics Class 2 Surface plasmon polaritons.
Nanowire dye-sensitized solar cells
LECTURE- 5 CONTENTS  PHOTOCONDUCTING MATERIALS  CONSTRUCTION OF PHOTOCONDUCTING MATERIALS  APPLICATIONS OF PHOTOCONDUCTING MATERIALS.
From weak to strong coupling of quantum emitters in metallic nano-slit Bragg cavities Ronen Rapaport.
A New Design Tool for Nanoplasmonic Solar Cells using 3D Full Wave Optical Simulation with 1D Device Transport Models Liming Ji* and Vasundara V. Varadan.
Applications of Photovoltaic Technologies. 2 Solar cell structure How a solar cell should look like ?  It depends on the function it should perform,
Properties of Photonic and Plasmonic Resonance Devices Jae Woong Yoon, Kyu Jin Lee, Manoj Niraula, Mohammad Shyiq Amin, and Robert Magnusson Dept. of Electrical.
Taming light with plasmons – theory and experiments Aliaksandr Rahachou, ITN, LiU Kristofer Tvingstedt, IFM, LiU , Hjo.
Surface polaritons in layered semiconductor structures M. Duracz, A. Rusina. Saint-Petersburg State Polytechnical University, Saint-Petersburg, Russia.
Surface Plasmon Spectroscopy Lokanathan Arcot Department of Forest Products Technology School of Chemical Technology Aalto University.
Beam manipulation via plasmonic structure Kwang Hee, Lee Photonic Systems Laboratory.
Wei E.I. Sha, Wallace C.H. Choy, and Weng Cho Chew
Boris N. Chichkov Leibniz University Hannover
Lavinia P. Rajahram 18 th April 2014 NANO LASER. SHRINKING THE LASER!
Cell and module construction. Photovoltaic effect and basic solar cell parameters To obtain a potential difference that may be used as a source of electrical.
EE 230: Optical Fiber Communication Lecture 11 From the movie Warriors of the Net Detectors.
Solar Cell Operation Key aim is to generate power by:
Fiona Beck Small Particles, Big Hopes: Absorption Enhancement in Silicon using Metallic Nanoparticles.
A-Si:H application to Solar Cells Jonathon Mitchell Semiconductors and Solar Cells.
Introduction: Optical Microscopy and Diffraction Limit
Plasmon enhanced thin-film solar cells: Advanced theoretical analysis and ellipsometric characterization Supervisor: Jesper Jung Postdoc
SURFACE PLASMON POLARITONS. SPPs Pioneering work of Ritchie (1957) Propagate along the surface of a conductor Trapped on the surface because of their.
Broad-band nano-scale light propagation in plasmonic structures Shanhui Fan, G. Veronis Department of Electrical Engineering and Ginzton Laboratory Stanford.
1 Surface Enhanced Fluorescence Ellane J. Park Turro Group Meeting July 15, 2008.
An Introduction to Quantum Dot Spectrometer Amir Dindar ECE Department, University of Massachusetts, Lowell.
Coupling of InGaN quantum-well photoluminescence to silver surface plasmons PRB, Vol 60, No 16, Pg Gontijo, M. Boroditsky, and E. Yablonovitch,UCLA.
The effects of global pollution on solar power efficiency Tom Hanley April 19, 2004.
Overview of course Capabilities of photonic crystals Applications MW 3:10 - 4:25 PMFeatheringill 300 Professor Sharon Weiss.
胡淑芬個人小檔案 1 /60. The Nanoscale ■ m = 1 Ångstrom ■ m = 1 Nanometer ■ m = 1 Micrometer ■ m = 1 Millimeter 2 /60.
Alternative Energy Sources Organic Photovoltaic (OPV) Timothy McLeod Summer 2006.
Waveguide High-Speed Circuits and Systems Laboratory B.M.Yu High-Speed Circuits and Systems Laboratory 1.
Brad Gussin John Romankiewicz 12/1/04 Quantum Dots: Photon Interaction Applications.
Interplay of polarization fields and Auger recombination in the efficiency droop of nitride light-emitting diodes APPLIED PHYSICS LETTERS 101, (2012)
Modeling Plasmonic Effects in the Nanoscale Brendan McNamara, Andrei Nemilentsau and Slava V. Rotkin Department of Physics, Lehigh University Methodology.
Nanoplasmonic structures: Designing electromagnetic fields
Surface Plasmons What They Are, and Their Potential Application in Solar Cells Martin Kirkengen, AMCS, UiO Collaboration with Joakim Bergli, Yuri Galperin,
Yibin Xu National Institute for Materials Science, Japan Thermal Conductivity of Amorphous Si and Ge Thin Films.
EM scattering from semiconducting nanowires and nanocones Vadim Karagodsky  Enhanced Raman scattering from individual semiconductor nanocones and nanowires,
Solar Cells Solar cells are made of two types of silicon Normal silicon has no free electrons N-type silicon has been doped with phosphorus to give it.
Itoh Lab. M1 Masataka YASUDA
Pellin Plasmonic Photocathodes Cherenkov Radiation Photocathode h  -> e- β = v p / c 1.Ag Particles 2.Ag Arrays 3.Ag Films.
Module 2/7: Solar PV Module Technologies. Module 1 : Solar Technology Basics Module 2: Solar Photo Voltaic Module Technologies Module 3: Designing Solar.
Light trapping with particle plasmons Kylie Catchpole 1,2, Fiona Beck 2 and Albert Polman 1 1 Center for Nanophotonics, FOM Institute AMOLF Amsterdam,
Surface Plasmon Resonance
Nanotechnology Application for Solar Cells: Using Quantum Dots to Modify Absorption Properties QUANTUM NANOS INC.
Universitetet i Oslo University of Oslo AMKS Group Surface Plasmons and Solar Cells M. Kirkengen, J. Bergli, Yu. M. Galperin Surface Plasmons Solar Cell.
BOC tutorial 12/10/2015. Wood, R W Philosophical Magazine 4: 269–275. angle grating silver Wavelength (Å) Angle of Incidence.
Penetration Depth & Reflectivity
Nanolithography Using Bow-tie Nanoantennas Rouin Farshchi EE235 4/18/07 Sundaramurthy et. al., Nano Letters, (2006)
Extremely thin solar absorbers Martijn de Sterke.
Hybrid states of Tamm plasmons and exciton-polaritons M Kaliteevski, S Brand, R A Abram, I Iorsh, A V Kavokin, T C H Liew and I A Shelykh.
Simulating Nanoscale Optics in Photovoltaics with the S-Matrix Method Dalton Chaffee, Xufeng Wang, and Peter Bermel Purdue University.
UPM, DIAC. Open Course. March EMITTERS AND PDs 8.1 Emitter Basics 8.2 LEDs and Lasers 8.3 PD Basics 8.4 PD Parameters 8.5 Catalogs.
NANO SCIENCE IN SOLAR ENERGY
MULTIFUNCTIONAL FIBER SOLAR CELLS USING TIO 2 NANOTUBES, PbS QUANTUM DOTS, AND POLY(3-HEXYLTHIOPHENE) by Dibya Phuyal MS Electrical Engineering EE 230.
My research topics related to surface plasmon
Surfaceplasmons in solar power Enhancing Efficiency of Solar Cells and Solar Thermal Collectors with surface Plasmon Resonances in Metal Nanoparticles.
Bandgap (eV) Lattice Constant (Å) Wavelength ( ㎛ ) GaN AlN InN 6H-SiC ZnO AlP GaP AlAs.
Physical concept Conclusions A gradient-index meta-surface is the very bridge to link PWs and SWs. Besides obvious interest in fundamental science, our.
Date of download: 7/9/2016 Copyright © 2016 SPIE. All rights reserved. Reference glass substrates (a) total transmission (b) and refractive index. Figure.
Nanodome Solar Cells with Efficient Light Management and Self-Cleaning
Possible methods of circumventing the 31% efficiency limit for thermalized carriers in a single–band gap absorption threshold solar quantum.
Plasmonic waveguide filters with nanodisk resonators
Harnessing Surface Plasmon Subwavelength Optics in Metallic Nanostructures for Enhanced Efficiency in Thin-Film Solar Cells Sang-Hyun Oh, Department of.
Solar cells Yogesh Wakchaure.
Solar cells Yogesh Wakchaure.
PRINCIPLE AND WORKING OF A SEMICONDUCTOR LASER
PLASMONICS AND ITS APPLICATIONS BY RENJITH MATHEW ROY. From classical fountations to its modern applications
Presentation transcript:

A brief overview of Plasmonic Nanostructure Design for Efficient Light Coupling into Solar Cells V.E. Ferry, L.A. Sweatlock, D. Pacifici, and H.A. Atwater, Nano Letters, Douglas Detert EE235 Prof. Connie Chang March 2, 2009

Douglas Detert — EE235 — March 2, 2009 Solar Cell Design/Material Considerations Conventional solar cells (e.g. Silicon) require thick absorption layers for complete absorption Thin film solar cells (e.g. CdTe, CIGS) decrease bulk recombination effects and allow for higher quality absorber materials Problem: Thin film cells are limited by decreased absorption, carrier excitation, and photocurrent Solution: Texture top/bottom surfaces to enhance light absorption

Douglas Detert — EE235 — March 2, 2009 Surface Plasmon Polariton Enhanced Solar Cells Surface Plasmon Polaritons (SPPs) are collective oscillations of free electrons at metal/dielectric boundaries SPPs are highly localized to interfaces and propagate easily for microns. Energy in SPP modes enhances absorption Momentum mismatch between incident light and SPPs does not allow for direct excitation of SPPs Goal: Design a nanostructure back contact that scatters light into SPP mode Barnes. J Opt A-Pure Appl Op 8 S87-S93 (2006)

Douglas Detert — EE235 — March 2, 2009 Scattering From a Single Groove Light energy is scattered into two key modes Photonic (~semiconductor) SPP (~interface) Both enhance photoabsorption, but photonic modes are not supported in extremely thin structures HyHy

Douglas Detert — EE235 — March 2, 2009 Results: Scattering From a Single Groove Finite-difference time-domain (FDTD) simulations paired with modal decomposition analysis Three physical effects involved in incoupling efficiencies: Fabry-Pérot resonance of thin film Photonic mode excitation at SPP resonance wavelength Polarization resonance of scatterer Film thickness and scatterer geometry affect above properties

Douglas Detert — EE235 — March 2, 2009 Effect of Groove Dimensions Groove width: SPP modes break down at large groove sizes, photonic mode flattens out Groove depth has little effect on incoupling efficiency Ridge-like structure: enhances photonic mode

Douglas Detert — EE235 — March 2, 2009 Conclusion & Outlook Groove-like nanostructures improve photoabsorption in thin film solar cells by coupling light to various modes, including interfacial SPP modes. Incoupling to SPP modes allows for enhancement in thin film solar cells To date, solar cells enhanced by SPPs have been fabricated with only top-layer patterning. Pillai et al. JAP (2007)