Planar Chiral Metamaterials & their application to optoelectronics devices W. Zhang, A. Papakostas, A. Potts, D. M. Bagnall, N. I. Zheludev Microelectronic.

Slides:



Advertisements
Similar presentations
24.6 Diffraction Huygen’s principle requires that the waves spread out after they pass through slits This spreading out of light from its initial line.
Advertisements

Thin Films, Diffraction, and Double slit interference
Vapor-deposited thin films with negative real refractive index in the visible regime J. J. Yi, A. Lakhatakia, W. Y. Ching, T.L. Chin Optics Express Vol.
Chris A. Mack, Fundamental Principles of Optical Lithography, (c) 2007
Measuring film thickness using Opti-Probe
Optical Activity Enantiomers are different compounds:
Digital Micromirror Devices for rapid fabrication of large-area laser- ablated multicolour-grating patterns B. Mills, D. J. Heath, M. Feinaeugle, R. W.
Properties of optically active compounds. Glucose is an optically active compound. On the straight-chain form of glucose shown here, all four of the carbons.
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.
Spectroscopic Ellipsometry University of Texas at El Paso Lynn Santiago Dr. Elizabeth Gardner Chem 5369.
Anton Samusev JASS’05 30 March – 9 April, 2005 Saint Petersburg State Polytechnical University, Ioffe Physico-Technical Institute Polarization effects.
Light and Optics 4.1 Mirrors form images by reflecting light. 4.2
1 Extreme Ultraviolet Polarimetry Utilizing Laser-Generated High- Order Harmonics N. Brimhall, M. Turner, N. Herrick, D. Allred, R. S. Turley, M. Ware,
In the name of God Photonic crystals created by holography Raheleh Mohammadpour.
Properties of Multilayer Optics An Investigation of Methods of Polarization Analysis for the ICS Experiment at UCLA 8/4/04 Oliver Williams.
PHY 1371Dr. Jie Zou1 Chapter 38 Diffraction and Polarization (Cont.)
Are you getting the concept? Calculate D a, D l, R d and s g for 1 st order diffraction under optimal conditions for the indicated 0.5 m grating with 100.
Negative Index/Refraction & Fabrication + Application EE235 2 nd presentation May 4 th, 2009 Jun Rho.
Metamaterial Emergence of novel material properties Ashida Lab Masahiro Yoshii PRL 103, (2009)
Chirality Bettelheim, Brown, Campbell and Farrell Chapter 15.
Overview of course Capabilities of photonic crystals Applications MW 3:10 - 4:25 PMFeatheringill 300 Professor Sharon Weiss.
Optical Characterization of GaN-based Nanowires : From Nanometric Scale to Light Emitting Devices A-L. Bavencove*, E. Pougeoise, J. Garcia, P. Gilet, F.
Waveguide High-Speed Circuits and Systems Laboratory B.M.Yu High-Speed Circuits and Systems Laboratory 1.
Daily Challenge, 1/7 If light is made of waves and experiences interference, how will the constructive and destructive interference appear to us?
Realization of an All-Dielectric Zero-Index Optical Metamaterial P. Moitra, Y. Yang, Z.Anderson, I.I.Kravchenko, D.B.Briggs, J.Valentine, Nature Photonics,
Resistless Fabrication of Embedded Nanochannels by FIB Patterning, Wet Etching and Atomic Layer Deposition Zhongmei Han Marko Vehkamaki Markku Leskelä.
1 Stereoisomerism Chapter 26 Hein * Best * Pattison * Arena Colleen Kelley Chemistry Department Pima Community College © John Wiley and Sons, Inc. Version.
BROOKHAVEN SCIENCE ASSOCIATES BIW ’ 06 Lepton Beam Emittance Instrumentation Igor Pinayev National Synchrotron Light Source BNL, Upton, NY.
PHENOMENA OF LIGHT Chapters 27, 29, & 31. Easy to get mixed up… Polarization (Light)Ch 27 Reflection (Water & Light)Ch 29 Refraction (Light)Ch 29 Dispersion.
FEMTOSECOND LASER FABRICATION OF MICRO/NANO-STRUCTURES FOR CHEMICAL SENSING AND DETECTION Student: Yukun Han MAE Department Faculty Advisors: Dr. Hai-Lung.
WAVEPLATES PLATE RETARDERS. A wave plate or retarder is an optical device that alters the polarization state of a light wave traveling through it. Waveplate.
Achromatic waveplate in THz frequency region based on the structured parallel metal plates Ashida Lab Noriyuki Mukai.
Properties of Chiral Molecules: Optical Activity
 Top DBR mirror replaced with CTF and chiral STF bilayers  The CTF (QWP) introduces a pi/2 retardance to compensate the polarization mismatch between.
Goal: To understand light Objectives: 1)To learn about the Properties of light 2)To learn about Diffraction 3)To learn about Polarization 4)To learn how.
 Is an instrumental analytical method using rotation of polarized light by some substances as measure of their concentration in a solution.  The instrument.
EE235 Presentation I CNT Force Sensor Ting-Ta YEN Feb Y. Takei, K. Matsumoto, I. Shimoyama “Force Sensor Using Carbon Nanotubes Directly Synthesized.
Today’s topic Alignment Polarization Mechanism 1.
Anne-Laure Fehrembach, Fabien Lemarchand, Anne Sentenac,
Lithography. MAIN TYPES OF LITHOGRAPHY: * Photolithography * Electron beam lithography –X-ray lithography –Focused ion beam lithography –Neutral atomic.
Self-assembly Nanostructure and Lithography
Philosophical Transactions A
Class overview: Brief review of physical optics, wave propagation, interference, diffraction, and polarization Introduction to Integrated optics and integrated.
1.Stable radiation source 2.Wavelength selector 3.Transparent sample holder: cells/curvettes made of suitable material (Table 7- 2) 4.Radiation detector.
Conditions for Interference
Single photon counting detector for THz radioastronomy. D.Morozov 1,2, M.Tarkhov 1, P.Mauskopf 2, N.Kaurova 1, O.Minaeva 1, V.Seleznev 1, B.Voronov 1 and.
2. Design Determine grating coupler period from theory: Determine grating coupler period from theory: Determine photonic crystal lattice type and dimensions.
LITHOGRAPHY IN THE TOP-DOWN PROCESS - BASICS
Diffraction (6.161 Lab3) Tony Hyun Kim 10/21/2008.
Nanolithography Using Bow-tie Nanoantennas Rouin Farshchi EE235 4/18/07 Sundaramurthy et. al., Nano Letters, (2006)
MIMTY 4/4/11 How would your life change if there were no lenses or mirrors? MIMTY.
Metal-insulator-metal metamaterial absorbers consisting of proximity-coupled resonators with the control of the fundamental and the second-order frequencies.
High performance optical absorber based on a plasmonic metamaterial 岑剡.
Date of download: 5/30/2016 Copyright © 2016 SPIE. All rights reserved. Working principle of the immersion schemes: (a) focusing in air, (b) focusing through.
Narrow-band filtering with resonant gratings under oblique incidence Anne-Laure Fehrembach, Fabien Lemarchand, Anne Sentenac, Institut Fresnel, Marseille,
0 Frequency Gain 1/R 1 R 2 R 3 0 Frequency Intensity Longitudinal modes of the cavity c/L G 0 ( ) Case of homogeneous broadening R2R2 R3R3 R1R1 G 0 ( )
All-Dielectric Metamaterials: A Platform for Strong Light-Matter Interactions Jianfa Zhang* (College of Optoelectronic Science and Engineering, National.
LIGHT BACKSCATTERING ANALYSIS of Textured Silicon SAMPLES
Internal CDR meeting December 20th, 2005
Two-layer ultra-high density x-ray optical memory (X-ROM)
Polarization and nonlinear effects enhancement in periodic structures and systems with strong field localization.
Luminescent Periodic Microstructures for Medical Applications
ASPERA Technology Forum 20/10/2011
Stereochemistry Stereochemistry refers to the
Optical Isomers.
ENANTIOMERIC PAIR mirror images NOT superimposable
Transverse coherence and polarization measurement of 131 nm coherent femtosecond pulses from a seeded FEL J. Schwenke, E. Mansten, F. Lindau, N. Cutic,
Fig. 4 Giant optical chirality.
Planar gradient meta-surface to focus EM waves in reflection geometry
Fig. 3 Wavelength and polarization tunable mirrorless lasing from the heliconical superstructure. Wavelength and polarization tunable mirrorless lasing.
Presentation transcript:

Planar Chiral Metamaterials & their application to optoelectronics devices W. Zhang, A. Papakostas, A. Potts, D. M. Bagnall, N. I. Zheludev Microelectronic Research Group School of Electronics and Computer Science University of Southampton

Overview Introduction Device design and fabrication Experimental setup Results Applications Conclusions Presenting Author : Wen Zhang

Introduction - 3D chirality Presenting Author : Wen Zhang A chiral carbon atom and its mirror image. Asymmetrical Enantiomers

2D chirality Triangle (a) and triangle (b) cannot be superimposed by any displacement in the plane. Reflection line (a) (b) Trying to superimpose (a) and (b) Presenting Author : Wen Zhang

Aim of the project Presenting Author : Wen Zhang Polarization rotation Reciprocity 3D chirality 2D chirality Yes ?

ξ ξ α -α-α ξ – Arm length α – Bending angle 2D gammadions design Presenting Author : Wen Zhang

Samples fabrication (a) Patterned aluminium gammadion on an electrically isolating buffer layer of polymeric material (b) Patterned Ti/Au/Ti “sandwich” multilayer gammadion structures Silicon substrate 300 nm UVIII resist Silicon substrate 50 nm Al Silicon substrate (a) 20 nm Ti 100 nm Au 20 nm Ti Silicon substrate Chiral shaped grooves etched into metallic films Silicon substrate UVIII photoresist (b)

Presenting Author : Wen Zhang Enantiomeric gammadion pair with a bending angle of ± 45º Enantiomeric gammadion pair with a bending angle of ± 90º Arm length ξ= 1.4μm, line width= 300~400nm

Experimental Setup Presenting Author : Wen Zhang Polarization state characterization Intensity measurement Polarimeter head Gammadion sample Focus lens Power meter 1 st -order reflected beam Laser source Quarter wave plate Linear polarizer Circular polarized light Linear polarized light

Presenting Author : Wen Zhang   Diffracted beam Polarization state  Planar chiral structure Plane of incidence   Incident Beam Polarization state  

Optical characterization of planar chiral metamaterials Presenting Author : Wen Zhang Polarization state dependence Intensity dependence

1 st Order diffraction from aluminium metallic planar chiral grating: polarization azimuth rotation Presenting Author : Wen Zhang Pure Al

1 st Order diffraction from aluminium metallic planar chiral grating: Ellipticity Presenting Author : Wen Zhang

1 st Order diffraction from aluminium metallic planar chiral grating: Intensity Presenting Author : Wen Zhang

Future application of planar chiral metamaterials Presenting Author : Wen Zhang Polarization sensitive modulators Polarization sensitive filters Polarization sensitive photodetectors

Polarization sensitive photodetector Presenting Author : Wen Zhang P+ anode contact P+ anode contact Top view C A N+ silicon P-sub Diffused n-silicon p+ n+ Cross-section Planar chiral structures

Conclusion Presenting Author : Wen Zhang Chirality & Handedness Optoelectronics devices Planar Chiral Metamaterials Strong polarization effect Intensity dependence Handedness polarization dependence