Passage of magnetostatic waves through the lattice on the basis of the magnon crystal. Performed by Lanina Mariya, III year student, Faculty of Nonlinear.

Slides:



Advertisements
Similar presentations
One-Dimensional Scattering of Waves 2006 Quantum MechanicsProf. Y. F. Chen One-Dimensional Scattering of Waves.
Advertisements

RF Communication Circuits
Frequency modulation and circuits
Light Waves and Polarization Xavier Fernando Ryerson Communications Lab
Study of propagative and radiative behavior of printed dielectric structures using the finite difference time domain method (FDTD) Università “La Sapienza”,
Mikhail Rybin Euler School March-April 2004 Saint Petersburg State University, Ioffe Physico-Technical Institute Photonic Band Gap Structures.
Shaping the color Optical property of photonic crystals Shine.
Lecture 6. Chapter 3 Microwave Network Analysis 3.1 Impedance and Equivalent Voltages and Currents 3.2 Impedance and Admittance Matrices 3.3 The Scattering.
Common Volume Multiplexing Technigues Coupled Wave Theory Derivation of Angular Selectivity Experimental Study of Angular Selectivity Optimum Beam Ratio.
1 Chapter 40 Quantum Mechanics April 6,8 Wave functions and Schrödinger equation 40.1 Wave functions and the one-dimensional Schrödinger equation Quantum.
ENE 428 Microwave Engineering
Bloch Oscillations Alan Wu April 14, 2009 Physics 138.
Chaos course presentation: Solvable model of spiral wave chimeras Kees Hermans Remy Kusters.
Thermally Deformable Mirrors: a new Adaptive Optics scheme for Advanced Gravitational Wave Interferometers Marie Kasprzack Laboratoire de l’Accélérateur.
Derivation of the Gaussian plume model Distribution of pollutant concentration c in the flow field (velocity vector u ≡ u x, u y, u z ) in PBL can be generally.
Instructor: Engr. Zuneera Aziz Course: Microwave Engineering
Chapter 5 Solutions for Interacting Waves Using A MCM 5.1 Governing Equations and Hierarchy Eq.s 5.2 An Example of Applying A Mode Coupling Method (MCM)
May 25, 2007Bilkent University, Physics Department1 Optical Design of Waveguides for Operation in the Visible and Infrared Mustafa Yorulmaz Bilkent University,
ElectroScience Lab IGARSS 2011 Vancouver Jul 26th, 2011 Chun-Sik Chae and Joel T. Johnson ElectroScience Laboratory Department of Electrical and Computer.
Modeling light trapping in nonlinear photonic structures
Lecture 8 Periodic Structures Image Parameter Method
ENE 311 Lecture 2. Diffusion Process The drift current is the transport of carriers when an electric field is applied. There is another important carrier.
ABOVE BARRIER TRANSMISSION OF BOSE-EINSTEIN CONDENSATES IN GROSS- PITAEVSKII APPROXIMATION Moscow, H.A. Ishkhanyan, V.P. Krainov.
Transmission Line Theory
Lecture 7. Tunable Semiconductor Lasers What determines lasing frequency: Gain spectrum A function of temperature. Optical length of cavity Mirror reflectance.
A. Krawiecki , A. Sukiennicki
1 Investigation of Optical Properties n, k … index of refraction and damping  1,  2 … polarization and absorption Problems: The penetration depth of.
Abstract Although the sine-Gordon equation was originally obtained for the description of four wave-mixing in transmission geometry, it describes self-diffraction.
In the absence of sources, the Maxwell equations in an infinite medium are.
The Propagation of Electromagnetic Wave in Atmospheric Pressure Plasma Zhonghe Jiang XiWei Hu Shu Zhang Minghai Liu Huazhong University of Science & Technology.
Electronic Band Structures electrons in solids: in a periodic potential due to the periodic arrays of atoms electronic band structure: electron states.
BIOPHYS: A Physically-based Algorithm for Inferring Continuous Fields of Vegetative Biophysical and Structural Parameters Forrest Hall 1, Fred Huemmrich.
TECHNOLOGICAL EDUCATIONAL INSTITUTE OF CENTRAL MACEDONIA DEPARMENT OF INFORMATICS & COMMUNICATIONS Master of Science in Communication.
Operated by JSA for the U.S. Department of Energy Thomas Jefferson National Accelerator Facility 1 Lecture 5  Magnetic Multipoles Magnetic Multipoles,
Lecture 5.
1 Challenge the future The Lateral Motion of Wafer under the Influence of Thin-film Flow Leilei Hu Solid and Fluid Mechanics
1 ENE 428 Microwave Engineering Lecture 11 Excitation of Waveguides and Microwave Resonator.
Transverse optical mode in a 1-D chain J. Goree, B. Liu & K. Avinash.
Nonlinear Optics Lab. Hanyang Univ. Chapter 6. Processes Resulting from the Intensity-Dependent Refractive Index - Optical phase conjugation - Self-focusing.
LATHE VIBRATIONS ANALYSIS ON SURFACE ROUHHNESS OF MACHINED DETAILS LATHE VIBRATIONS ANALYSIS ON SURFACE ROUHHNESS OF MACHINED DETAILS * Gennady Aryassov,
ONE-DIMENSIONAL ANALYSIS ON BEDEVOLUTION ACCOMPANING BANK EROSION Satoru Nakanishi Hokkaido University Graduate School Kazuyoshi Hasegawa Hokkaido University.
COHERENT BREMSSTRAHLUNG OF RELATIVISTIC ELECTRONS UNDER THE EXTERNAL ACOUSTIC FIELD A.R. Mkrtchyan Institute of Applied Problems in Physics, NAS, Armenia.
Photonic band gaps in 12-fold symmetric quasicrystals B. P. Hiett *, D. H. Beckett *, S. J. Cox †, J. M. Generowicz *, M. Molinari *, K. S. Thomas * *
Modelling and Simulation of Passive Optical Devices João Geraldo P. T. dos Reis and Henrique J. A. da Silva Introduction Integrated Optics is a field of.
Collin Broholm Johns Hopkins University and NIST Center for Neutron Research Quantum Phase Transition in Quasi-two-dimensional Frustrated Magnet M. A.
Spin Wave Model to study multilayered magnetic materials Sarah McIntyre.
Ferrite measurements of Mu2e AC dipole Summer Student Meeting August 25, 2010 Student: Evgeny Bulushev, NSU Supervisor: George Velev, TD\Magnet Systems.
Collin Broholm Johns Hopkins University and NIST Center for Neutron Research Quantum Phase Transition in Quasi-two-dimensional Frustrated Magnet M. A.
Linac RF System Design Options Y. Kang RAD/SNS/NScD/ORNL Project – X Collaboration Meeting April , 2011.
Date of download: 7/5/2016 Copyright © 2016 SPIE. All rights reserved. Basic principle of the proposed circuit. The lower portion of the figure contains.
Microwave Engineering by David M. Pozar Ch. 4.1 ~ 4 / 4.6
Radio Coverage Prediction in Picocell Indoor Networks
Focusing performance of a bent polychromator crystal with coincidence of the polychromatic and dynamical focusing effects Symmetric transmission geometry.
Light propagation in topological two-level structures
Surface acoustic waves control with external magnetic field in TbCo2/FeCo films Vladimir Onoprienko,1, 2, 3 Ivan Lisenkov,1, 2, 3, Alexey Klimov,1, 2,
THE METHOD OF LINES ANALYSIS OF ASYMMETRIC OPTICAL WAVEGUIDES Ary Syahriar.
Maksim Skorobogatiy John Joannopoulos MIT, Department of Physics
topics Basic Transmission Line Equations
ENE 428 Microwave Engineering
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
Wireless Communications Chapter 4
A THEORETICAL MODEL for MAGNETIC FIELD IMAGING with “SWISS ROLLS” STRUCTURES V. Yannopapas J. B. Pendry M. C. K. Wiltshire J. Hajnal.
Energy Band 7 In free electron model, electrons occupy positive energy levels from E=0 to higher values of energy. They are valence electron so called.
ENE 428 Microwave Engineering
Magnetic Multipoles, Magnet Design
ENE 428 Microwave Engineering
Antenna Theory Chapter.4.7.4~4.8.1 Antennas
Chapter 8.1 Chapter 8.2 PERIODIC STRUCTURES
2nd Week Seminar Sunryul Kim Antennas & RF Devices Lab.
Presentation transcript:

Passage of magnetostatic waves through the lattice on the basis of the magnon crystal. Performed by Lanina Mariya, III year student, Faculty of Nonlinear Processes, Saratov State University. Supervisor: Ph.D. Sharaevsky J.P., Head of the Department of Nonlinear Physics, Faculty of Nonlinear Processes, Saratov State University 5th Helmholtz International Summer School - Workshop Dubna International Advanced School of Theoretical Physics - DIAS TH Calculations for Modern and Future Colliders July 23 - August 2, 2012, Dubna, Russia

Magnon crystals are the structures, similar to photonic crystals, but created on the basis of magnetic materials in which propagating waves are spin waves. In terms of application - the development of tunable magnetic field devices of information processing in the microwave range. Examples of 1-D and 2-D magnon crystals

The purpose : The contents of the report: 1. The scheme of analysis and the basic relations. 2. The calculation of the reflectivity of the crystal lattice on the magnon crystal. 3. Comparison with the experiment. 4. Nonlinear properties of the magnon crystal. Building a model based on the method of coupled modes for the description of the propagation of magnetostatic waves through the lattice on the basis of one- dimensional analysis of the magnon crystal and the reflectivity of the lattice, depending on the geometry of the structure.

Brillouin diagram: Bragg condition: where - Bragg frequency corresponding to the center frequency of the band gap.,

Diagram of the structure: – period, – width of the protrusion, - film thickness, – height of the projection. The dispersion equation for SMSW: where and ( - gyromagnetic ratio; - the saturation magnetization); -frequency; - the propagation constant of SMSW.,

The equations for the forward and backward waves : - slowly varying amplitudes of forward and backward waves, respectively. where The Fourier component of the magnetostatic potential: synchronism condition: and The distribution of the magnetostatic potential : и - the coupling coefficient. - detuning from the Bragg wave number.

Coupled-mode equations :, looking for the solution of the system in the form : dispersion equation : If passband band gap is real is imaginary

Basic relations: Reflection coefficient: Reflectivity: Phase of reflection coefficient : Transmittance :

Calculation of the reflectivity and phase

Calculation of the reflectivity.

The experimental frequency response of one-dimensional magnon crystal Theoretical dependence for one-dimensional magnon crystal

Nonlinear coupled-mode equations, We are searching for the solution of the form: where- coefficient of nonlinearity. Introduce- this parameter shows how the total power is divided between direct and counter-propagating waves. - backward wave dominates - direct wave dominates,

The conclusions are: 1. The analysis of the reflectivity of the lattice on the basis of one-dimensional magnon crystal and the reflection coefficient was calculated from the geometric dimensions of the structure in the excitation of surface magnetostatic waves. It is shown that even when the ratio of the structure to its period is greater than or equal to seven the reflection coefficient achieves the value one. 2. A comparison of calculated results with experimental data. A good qualitative agreement of the results. 3. It is shown that with increasing level of input power band gap shifts to lower frequencies.