All-Optical Gyroscope Based on Sagnac Effect in Photonic Crystal Coupled Cavity Waveguides and Slow Light Structures Work published in: B.Z. Steinberg,

Slides:



Advertisements
Similar presentations
Slow light and resonance phenomena in photonic crystals
Advertisements

Rotation Induced Super Structure in Slow-Light Waveguides w Mode Degeneracy Ben Z. Steinberg Adi Shamir Jacob Scheuer Amir Boag School of EE, Tel-Aviv.
1 Coupled Cavity Waveguides in Photonic Crystals: Sensitivity Analysis, Discontinuities, and Matching (and an application…) Ben Z. Steinberg Amir Boag.
Enhanced Non-Reciprocity by Rotations Interplay: One-Way Plasmonic Chains and Perfectly Matched Nano-Antennas 1 Ben Z. Steinberg Yakir Hadad Yarden Mazor.
Ultrashort laser sources
Ring Laser Gyroscopes Micah Larson April 21, 2005.
1 SLOW LIGHT AND FROZEN MODE REGIME IN PHOTONIC CRYSTALS April, 2007 Alex Figotin and Ilya Vitebskiy University of California at Irvine Supported by MURI.
1 Frozen modes and resonance phenomena in periodic metamaterials October, 2006 Alex Figotin and Ilya Vitebskiy University of California at Irvine Supported.
SagNAC Interferometry
LVC Meeting 2009: AIC Workgroup: Shahriar / LIGO G Design constraints and optimization for a white light cavity based GW interferometer including.
Propagation of surface plasmons through planar interface Tomáš Váry Peter Markoš Dept. Phys. FEI STU, Bratislava.
Optical Field Mixing. Oscillating Polarisation Optical polarisation Fundamental polarisation SH Polarisation Constant (dc) polarisation.
Slow light in photonic crystal waveguides Nikolay Primerov.
Cavity decay rate in presence of a Slow-Light medium
Tutorial on optical fibres F. Reynaud IRCOM Limoges Équipe optique F. Reynaud IRCOM Limoges Équipe optique Cargèse sept 2002.
Agilent Technologies Optical Interconnects & Networks Department Photonic Crystals in Optical Communications Mihail M. Sigalas Agilent Laboratories, Palo.
Lecture 1 Review of Wave optics Today Introduction to this course Light waves in homogeneous medium Monochromatic Waves in inhomogeneous medium.
Optical Gyroscope Arman Cingoz 11/3/04. Outline Sagnac Effect Passive Ring Resonator Gyro (Fiber Gyro) Active Ring Resonator (Laser Gyro) Applications.
RING LASER GYROSCOPES Sagnac Effect
By Bhaskar Department of Physics K L University. Lecture 2 (28 July) Interference.
Lattice Vibrations, Part I
Modeling light trapping in nonlinear photonic structures
Photonic Crystals Photonics Research Laboratory
1 Sensitivity Analysis of Narrow Band Photonic-Crystal Waveguides and Filters Ben Z. Steinberg Amir Boag Ronen Lisitsin Svetlana Bushmakin.
Some of the applications of Photonic Crystals (by no means a complete overview) Prof. Maksim Skorobogatiy École Polytechnique de Montréal.
Interaction of radiation with atoms and ions (I) Absorption- Stimulated emission E1E1 E2E2 W 12 =W 21 Spontaneous emission More definitionsCross section.
Symmetry Figures are identical upon an operation Reflection Mirror Line of symmetry.
Optical Gyroscopes for Ground Tilt Sensing in Advanced LIGO The need for low frequency tilt sensing The optics in Advanced LIGO’s suspensions must be very.
1 Sagnac Effect in Rotating Photonic Crystal Micro-Cavities and Miniature Optical Gyroscopes Tel Aviv University Ben Z. Steinberg Ady Shamir Amir Boag.
Hanjo Lim School of Electrical & Computer Engineering Lecture 2. Basic Theory of PhCs : EM waves in mixed dielectric.
Propagation in Photonic Crystal Coupled Cavity Waveguides Possessing Discontinuities Ben Z. Steinberg Amir Boag Orli Hershkoviz Mark Perlson Tel Aviv University.
T’ = Dilated Time t = Stationary time V = velocity C = Speed of light.
EE 495 Modern Navigation Systems Inertial Sensors Monday, Feb 09 EE 495 Modern Navigation Systems Slide 1 of 19.
Atomic transitions and electromagnetic waves
Wave Physics PHYS 2023 Tim Freegarde.
Elements of electromagnetic field theory and guided waves
REVISION SOUND.
Left-handed Nuclei S. Frauendorf Department of Physics University of Notre Dame, USA IKH, Forschungszentrum Rossendorf Dresden, Germany.
Quantum mechanical properties of Bessel EM modes and their effect on atomic systems Rocio Jáuregui Renaud Instituto de Física, Universidad Nacional Autónoma.
Simple numerical scheme for modelling of nonlinear pulse propagation in coupled microring resonators Anna Sterkhova, Jiří Petráček, Jaroslav Luksch ICTON.
PONDEROMOTIVE ROTATOR: REQUIREMENTS Zach Korth (Caltech) – GWADW ‘12 – Waikoloa, HI.
EE 495 Modern Navigation Systems Inertial Sensors Wed, Feb 17 EE 495 Modern Navigation Systems Slide 1 of 18.
Strapdown Inertial Navigation Systems (INS) Sensors and UAVs Avionic
5. Electromagnetic Optics. 5.1 ELECTROMAGNETIC THEORY OF LIGHT for the 6 components Maxwell Eq. onde Maxwell.
Except otherwise noted, this work is licensed under a Creative Commons Attribution 4.0 International License. Modes in infinite slab waveguides ELEC-E3240.
Prof. dr. A. Achterberg, Astronomical Dept., IMAPP, Radboud Universiteit.
1D Kinematics Equations and Problems. Velocity The rate at an object changes position relative to something stationary. X VT ÷ x ÷
9/2/2015PHY 711 Fall Lecture 41 PHY 711 Classical Mechanics and Mathematical Methods 10-10:50 AM MWF Olin 103 Plan for Lecture 4: Chapter 2 – Physics.
Direct Observation of Polariton Waveguide in ZnO nanowire at Room Temperature motivation abstract We report the direct experimental evidence of polariton.
The Sagnac Effect and the Chirality of Space Time Prof. R. M. Kiehn, Emeritus Physics, Univ. of Houston Dimdim December.
Ring Resonator Gyroscope
PHYS 408 Applied Optics (Lecture 12)
Photonic Bandgap (PBG) Concept
Fiber Optic Gyroscope (FOG)
Remote tuning of an optical resonator
Basic properties of waves
Group Velocity and Ultrafast Optics
Maksim Skorobogatiy John Joannopoulos MIT, Department of Physics
الفصل 1: الحركة الدورانية Rotational Motion
Waves Electrons (and other particles) exhibit both particle and wave properties Particles are described by classical or relativistic mechanics Waves will.
Slow light in Photonic Crystals
Summary of Lecture 18 导波条件 图解法求波导模式 边界条件 波导中模式耦合的微扰理论
3-dB Couplers/splitters
Energy hn Photon Electron Frequency n “Size”? l = c/n momentum?
Maxwell’s Equations and Plane Wave
Classical Mechanics PHYS 2006 Tim Freegarde.
The equations for circular motion are identical to those of linear motion except for variable names. True False.
Rectangular Waveguide
Two-Plate Waveguide Wave impedance TM mode
Tailor the Angular Dispersion of Metasurfaces
Presentation transcript:

All-Optical Gyroscope Based on Sagnac Effect in Photonic Crystal Coupled Cavity Waveguides and Slow Light Structures Work published in: B.Z. Steinberg, ‘’Rotating photonic crystals: a medium for compact optical gyroscopes”, Phys. Rev. E, vol 71, pp. 056621-7, May 31 2005

Basic Principles A CCW folded back upon itself in a fashion that preserves symmetry Micro-cavities Stationary Rotating at angular velocity C - wise and counter C - wise propag are identical. “Conventional” self-adjoint formulation. Dispersion is the same as that of a regular CCW except for additional requirement of periodicity: Co-Rotation and Counter - Rotation propag DIFFER. E-D in accelerating systems; non self-adjoint Dispersion differ for Co-R and Counter-R: Two different directions

Formulation E-D in the rotating system frame of reference: We have the same form of Maxwell’s equations: But constitutive relations differ: The resulting wave equation is (first order in velocity):

Solution Procedure: Results: Tight binding theory Non self-adjoint formulation (Galerkin) Results: Dispersion: W0 Q w k km -km |W0 Q| Dw w (-km ; W0 ) w0 w (km ; W0 ) w (km ; W0 = 0 ) At rest Rotating Depends on system design

The Gyro application Measure beats between Co-Rot and Counter-Rot modes: Rough estimate: For Gyro operating at optical frequency and CCW with :