Optical Properties of Metal Nanoparticles

Slides:



Advertisements
Similar presentations
The Wave Nature of Light Thin Film Interference
Advertisements

Gold(Au) Nanoparticles (and silver)
T. Ozaki, K. Sugano, T. Tsuchiya, O. Tabata
Shaping the color Optical property of photonic crystals Shine.
Mikko Nisula Overview Introduction Plasmonics Theoretical modeling Influence of particle properties Applications.
Nanomaterial Properties Plasmonics, Lorentz Oscillator Model,
Gothic Cathedrals and Solar Cells (and maybe a Grail?) A short introduction to the phenomenon of Surface Plasmons and their role in the scattering of light.
The Propagation of Light
Dr. Rinat Ankri and Dr. Dror Fixler
Resonances and optical constants of dielectrics: basic light-matter interaction.
Plasmonics The long wavelength of light (≈  m) creates a problem for extending optoelectronics into the nanometer regime. A possible way out is the conversion.
Surface Plasmon Spectroscopy Lokanathan Arcot Department of Forest Products Technology School of Chemical Technology Aalto University.
Lavinia P. Rajahram 18 th April 2014 NANO LASER. SHRINKING THE LASER!
Surface-Enhanced Raman Scattering (SERS)
Astro 201: Sept. 14, 2010 Read: Hester, Chapter 4 Chaos and Fractal information on class web page On-Line quiz #3: available after class, due next Tuesday.
Fiber-Optic Communications James N. Downing. Chapter 2 Principles of Optics.
Week 10 – More E&M theory, attenuation, color.
Nonlinear Optics Lab. Hanyang Univ. Chapter 3. Classical Theory of Absorption 3.1 Introduction Visible color of an object : Selective absorption, Scattering,
Science and Technology of Nano Materials
Department of Electrical and Computer Engineering
Photochemistry And Photophysics Of Nanoparticles Brian Ellis.
UNIVERSITY OF KENTUCKY College of Engineering RADIATIVE TRANSFER LABORATORY Department of Mechanical Engineering Directed Melting.
The Hong Kong Polytechnic University Optics II----by Dr.H.Huang, Department of Applied Physics1 Light Waves Nature of Light: Light can be viewed as both.
Thin films The index of refraction (h) for a medium is defined as the speed of light in vacuum (c) divided by the speed of light in the medium(v).
Light Waves and Color Metro Community College 9/19/2015.
Attenuation by absorption and scattering
Optical Properties of Gold Nanoparticles
Surface Plasmons What They Are, and Their Potential Application in Solar Cells Martin Kirkengen, AMCS, UiO Collaboration with Joakim Bergli, Yuri Galperin,
1. Waves and Particles 2. Interference of Waves
1 Chapter 3 Electromagnetic Theory, Photons and Light September 5,8 Electromagnetic waves 3.1 Basic laws of electromagnetic theory Lights are electromagnetic.
Chapter 26 Properties of Light Electromagnetic Waves Traveling, oscillating, electric and magnetic fields which are emitted by vibrating charges. The.
Optics on a Nanoscale Using Polaritonic and Plasmonic Materials (NSF NIRT ) Andrey Chabanov 1, Federico Capasso 2, Vinothan Manoharan 2, Michael.
Nanoparticle Optics Part 1
Interference Introduction to Optics Coherent source Two Slit Interference Thin film interference Interference from a Grating.
PRESENT BY- RUCHI DIXIT KAMAKSHI KHATRI. INTRODUCTION During the last two decades we have witnessed remarkable research and development activity aimed.
Chapters: 3and 4. THREE MAIN LIGHT MATTER INTERRACTION Absorption: converts radiative energy into internal energy Emission: converts internal energy into.
Pellin Plasmonic Photocathodes Cherenkov Radiation Photocathode h  -> e- β = v p / c 1.Ag Particles 2.Ag Arrays 3.Ag Films.
Chapter 2 Properties on the Nanoscale
Surface Plasmon Resonance
Lecture 26-1 Lens Equation ( < 0 )  True for thin lens and paraxial rays.  magnification m = h’/h = - q/p.
Chapter 1 Introduction 1.1 Classification of optical processes Reflection Propagation Transmission Optical medium refractive index n( ) = c / v ( )
Nonlinear Optical Response of Nanocavities in Thin Metal Films Yehiam Prior Department of Chemical Physics Weizmann Institute of Science With Adi Salomon.
Introduction to materials physics #3
Lecture 21 Optical properties. Incoming lightReflected light Transmitted light Absorbed light Heat Light impinging onto an object (material) can be absorbed,
Penetration Depth & Reflectivity
LOSSES IN FIBER BY:Sagar Adroja.
BRIGHT NEW WORLD NORBERT KROO HUNGARIAN ACADEMY OF SCIENCES DUBNA,
Outline 1.Motivation1.Motivation 1.Theories1.Theories 2.Results and discussions2.Results and discussions 3.Future work3.Future work.
Saturable absorption and optical limiting
Optical thin films for high temperature gas sensing in advanced power plant applications Plasmon resonance of TiO 2 / Au at extreme temperatures Presented.
Introduction to Physics and Astronomy (1) 2-1. Light and Black Body Radiation.
Surface-Enhanced Raman Scattering (SERS)
기계적 변형이 가능한 능동 플라즈모닉 기반 표면증강라만분광 기판 Optical Society of Korea Winter Annual Meting 강민희, 김재준, 오영재, 정기훈 바이오및뇌공학과, KAIST Stretchable Active-Plasmonic.
Date of download: 6/26/2016 Copyright © 2016 SPIE. All rights reserved. Schematics of the considered systems: submonolayer film of NPs adsorbed on a dielectric.
List of Topics for Team Presentation Surface-enhanced Spectroscopy (100) Plasmonic Light Harvesting (150) Mie Theory (100)
Introduction of Nanoplasmonics 2011 Spring Semester.
Properties of Light Waves, particles and EM spectrum Interaction with matter Absorption Reflection, refraction and scattering Diffraction and polarization.
Chapter 25 Wave Optics.
Semiconductor Nanocrystals
The Dielectric Function of a Metal (“Jellium”)
Electromagnetic Waves
Trivia Question Human vision (in daylight) is based on three color receptors which are sensitive to Red, Green, and Blue light. Hence RGB monitors… How.
NANOCHEMISTRY.
Electromagnetic Waves
Chapter 25 Wave Optics Chapter 34 Opener. The beautiful colors from the surface of this soap bubble can be nicely explained by the wave theory of light.
Interference Introduction to Optics Coherent source
Electromagnetic Waves
Lecture 12 Optical Properties Md Arafat Hossain Outlines.
Optical properties of a conductor
PLASMONICS AND ITS APPLICATIONS BY RENJITH MATHEW ROY. From classical fountations to its modern applications
Presentation transcript:

Optical Properties of Metal Nanoparticles Sriharsha Karumuri

Introduction Why nanoparticles are different from bulk materials? Nanoparticles are different from bulk materials and isolated molecules because of their unique optical, electronic and chemical properties. As the dimensions of the material is reduced the electronic properties change drastically as the density of states and the spatial length scale of the electronic motion are reduced with decreasing size. Closely related to size-induced changes in the electronic structure are the optical properties of nanoparticles.

1) Gold nanoparticles were used as a pigment of ruby-colored stained glass dating back to the 17th century. Figure.1 shows a picture of the Rose Window of the Cathedral of Notre Dame. The bright red and purple colors are due to gold nanoparticles. 2) Lycurgus cup: It appears green in reflected light, but appears red when light is shone from inside, and is transmitted through the glass.

Surface plasmon resonance When a nanoparticle is much smaller than the wave length of light, coherent oscillation of the conduction band electrons induced by interaction with an electromagnetic field. This resonance is called Surface Plasmon Resonance (SPR). Figure: Schematic of plasmon oscillation for a sphere, showing the displacement of the conduction electron charge cloud relative to the nuclei.

Literature review Michael Faraday was first to report the study of the synthesis and colors of colloidal gold. In 1908, Mie explained this phenomenon by solving Maxwell’s equation. Mie theory predicted optical extinction of homogenous spherical particles 2R<<λ for very small particles as (extinction = scattering + absorption) Where as V is the particle volume, ω is the angular frequency of the exciting light, and c is the speed of light. εm and ε (ω) = ε1 (ω)+ ε 2 (ω) are the dielectric functions of the surrounding medium and the metal, respectively

Synthesis processes Wet chemical process Mechanical process Form in phase Gas phase synthesis Electroless deposition

Size dependence The changes gold–blue–purple–red are largely geometric ones that can be explained with Mie theory, which describes light-scattering by a sphere. When the metal nanoparticle is larger than the ~30 nm, the electrons oscillating with the light is not perfectly in phase. Some electrons get behind; this phenomenon is called retardation effect or phase retardation. The subsequent changes, reddish - brown to orange to colorless, are due to quantum size effects. Mulvaney, MRS Bulletin 26, 1009 (1996)

Surrounding medium The surface plasmon resonance peak changes with its own dielectric properties and those of its local environment including the substrate, solvent, and adsorbates. This principle that the high sensitivity of the surface plasmon resonance spectrum of noble metal nanoparticles to adsorbate-induced changes in the dielectric constant of the surrounding nanoenvironment used in chemosensing and biosensing. Spectral shift for individual blue (roughly spherical) silver nanoparticles. Typical blue particle spectrum as it is shifted from (a) air to (b) 1.44 index oil, and successive oil treatments in 0.04 index incremental increases. Jack J. Mock, David R. Smith, and Sheldon Schultz, Local Refractive Index Dependence of Plasmon Resonance Spectra from Individual Nanoparticles, Nano letters 2003 Vol. 3 No. 4 485-491.

Particle density Beginning from the left “glass is doped with gold nanoparticles” and spacing between them is large. In the right side figure ‘the bulk gold is doped with glass’. As the spacing is reduced, dipole interactions become increasingly important. (a) Transmitted colors of the same Au@SiO2 films. (b) The reflected color of the films after deposition from a ruby red gold sol as a function of the silica shell thickness. Top left going across: 15 nm gold particles coated with silica shells of thickness 17.5, 12.5, 4.6, 2.9, and 1.5 nm. Thearith Ung, Luis M. Liz-Marzan, and Paul Mulvaney, optical Properties of Thin Films of Au@SiO2 Particles, J. Phys. Chem. B 2001, 105, 3441-3452.

Applications These differences in properties of nanoparticles are used in microelectronics, quantum dot lasers, chemical sensors, data storage, and a host of other applications. Possible future applications of nanoparticles include the areas of ultrafast data communication and optical data storage, solar energy conversion, and the use of metallic nanoparticles as catalysts because of their high surface-to-volume ratios and different shapes.

QUESTIONS ???

THANK YOU