Sergey N. Galyamin, Andrey V. Tyukhtin

Slides:



Advertisements
Similar presentations
Motion of a Charged Particle in a Magnetic Field
Advertisements

NASSP Self-study Review 0f Electrodynamics
1 The Quantization of the Angular Momentum. 2 In the gas phase discrete absorption lines appear in the spectral reagions where in the liquid phase the.
1 General Properties of Electromagnetic Radiation Lecture 1.
Chapter 1 Electromagnetic Fields
Interaction of Electromagnetic Radiation with Matter
EEE 498/598 Overview of Electrical Engineering
So far Geometrical Optics – Reflection and refraction from planar and spherical interfaces –Imaging condition in the paraxial approximation –Apertures.
Introduction to Light IN THIS LECTURE –Light –Electromagnetic Radiation –Wave Nomenclature –Electromagnetic Spectrum –Speed of Light –Wave front and wave.
Evan Walsh Mentors: Ivan Bazarov and David Sagan August 13, 2010.
Physical Modeling, Fall THE MAGNETIC FIELD B is the symbol for the magnetic field. Magnetic field lines run from north poles to south poles. Like.
ELECTROMAGNETIC RADIATION
November 10, 2014 Jackson’s Electrodynamics Michelle While USD.
The Magnetic Field The force on a charge q moving with a velocity The magnitude of the force.
Lecture 14 (11/13/2006) Analytical Mineralogy Part 1: Nature of Light Introduction to Optical Mineralogy.
04/06/2015PHY 712 Spring Lecture 281 PHY 712 Electrodynamics 9-9:50 AM MWF Olin 103 Plan for Lecture 28: Continue reading Chap. 14 – Radiation.
1 Optical Properties of Materials … reflection … refraction (Snell’s law) … index of refraction Index of refraction Absorption.
17.1 The Nature of the Electromagnetic Waves
The Electromagnetic Field. Maxwell Equations Constitutive Equations.
Optical Mineralogy Technique utilizing interaction of polarized light with minerals Uses a polarizing microscope Oils - Grain mounts Thin sections – rocks.
Lattice Vibrations, Part I
AP Physics Chapter 20 Electromagnetic Induction. Chapter 20: Electromagnetic Induction 20.1:Induced Emf’s: Faraday’s Law and Lenz’s Law : Omitted.
O Aim of the lecture  Introduction of Waves water as a model Radio  Light representation with rays refraction reflection o Main learning outcomes  familiarity.
RAY-OPTICAL ANALYSIS OF RADIATION OF A CHARGE FLYING NEARBY A DIELECTRIC OBJECT Ekaterina S. Belonogaya, Sergey N. Galyamin, Andrey V. Tyukhtin Saint Petersburg.
Consider a time dependent electric field E(t) acting on a metal. Take the case when the wavelength of the field is large compared to the electron mean.
PROPAGATION OF SIGNALS IN OPTICAL FIBER 9/20/11. Light Characteristics Particle Characteristics Light has energy Photons are the smallest quantity of.
Light and Matter Tim Freegarde School of Physics & Astronomy University of Southampton Classical electrodynamics.
Measurements in Fluid Mechanics 058:180:001 (ME:5180:0001) Time & Location: 2:30P - 3:20P MWF 218 MLH Office Hours: 4:00P – 5:00P MWF 223B-5 HL Instructor:
Periodic Boundary Conditions in Comsol
and Accelerator Physics
Unit 9: Part 2 Electromagnetic Induction and Waves.
Miscellaneous Topics Curvature Radiation Cernkov Radiation.
Tatiana Yu. Alekhina and Andrey V. Tyukhtin Physical Faculty of St. Petersburg State University, St. Petersburg, Russia Radiation of a Charge in a Waveguide.
Fundamentals of wave kinetic theory
RADIATION OF A CHARGE FLYING FROM VACUUM INTO ANISOTROPIC DISPERSIVE MEDIUM Sergey N. Galyamin, Andrey V. Tyukhtin Radiophysics Department, Physical faculty,
PHY 712 Electrodynamics 9-9:50 AM MWF Olin 103 Plan for Lecture 36: Review Part II:  Further comment of Kramers-Kronig transform  Some equations for.
Powerpoint Templates Page 1 Powerpoint Templates Electromagnetic Radiation.
Neutrino quantum states and spin light in matter Neutrino motion and radiation in matter Neutrino quantum states and spin light in matter Alexander Studenikin.
Magnetic Field Lines Graphical Illustration of Magnetic Fields Lines start on north pole and end on south pole Opposite poles attract, like poles reply.
ELECTROMAGNETIC WAVES. Current can be induced in a coil by a changing magnetic field. A changing magnetic field induces a changing electric field at right.
5. Electromagnetic Optics. 5.1 ELECTROMAGNETIC THEORY OF LIGHT for the 6 components Maxwell Eq. onde Maxwell.
04/10/2015PHY 712 Spring Lecture 301 PHY 712 Electrodynamics 9-9:50 AM MWF Olin 103 Plan for Lecture 30: Finish reading Chap. 14 – Radiation from.
Waves in magnetized plasma
Powerpoint Templates Page 1 Powerpoint Templates Electromagnetic Radiation.
EE231 Introduction to Optics: Basic EM Andrea Fratalocchi ( slide 1 EE 231 Introduction to Optics Review of basic EM concepts Andrea.
Chapter 1 Electromagnetic Fields
Ionization losses by fast particles in matter, non-relativistic case
ELEC 401 MICROWAVE ELECTRONICS Lecture 2
А.V. Tyukhtin Saint-Petersburg State University
E or B? It Depends on Your Perspective
Lecture 3-5 Faraday’ s Law (pg. 24 – 35)
How an electromagnetic wave is produced
Electromagnetic Radiation
Review of basic EM concepts
Light Waves and Polarization
Review Lecture Jeffrey Eldred Classical Mechanics and Electromagnetism
Lienard Wierchert Potential
A vibration or disturbance that transfers energy.
WHAT IS A WAVE? disturbance that transports energy through matter or space.
(Based on medium) 2. Mechanical Waves
ELEC 401 MICROWAVE ELECTRONICS Lecture 2
General theory of scattering in isotropic media
Is charge moving?.
Review of basic EM concepts
LECTURE I: SINGLE-PARTICLE MOTIONS IN ELECTRIC AND MAGNETIC FIELDS
Optics 430/530, week II Plane wave solution of Maxwell’s equations
The Motion of Charged Particles in Magnetic Fields
Accelerator Physics Synchrotron Radiation
1st Week Seminar Sunryul Kim Antennas & RF Devices Lab.
Presentation transcript:

Electromagnetic Field of Charged Particle Bunches Moving in Gyrotropic Media Sergey N. Galyamin, Andrey V. Tyukhtin Saint Petersburg State University Physical faculty Radiophysics Department

Formulation of the problem gyrotropic (chiral) medium Anisotropic chiral medium Isotropic chiral medium Cold magnetized plasma Condon medium The problem statement is the following. We consider the cylindrical frame ro, phi, z. In the plane z=0 the interface between vacuum and uniaxial crystal is placed. A point charge q moves with constant velocity from vacuum into medium, the charge movement rule is the following. We suppose the crystal being nonmagnetic with the plasma frequency dispersion (with losses) of their components. As you can see, this is the classical formulation of the transition radiation problem. The question appears: “What is new here?” However the usual think which is analyzed in this problem is spectral-angle distribution of the radiated energy. But the main goal of this report is to investigate in detail the structure of the EMF with taking into account specific frequency dispersion and small losses. negligible losses

General theory Cold magnetized plasma Condon medium complex elliptical polarization right-hand circular polarization left-hand circular polarization

Cold magnetized plasma General theory Cold magnetized plasma Condon medium

General theory Cold magnetized plasma Condon medium Asymptotic properties of integrands SDP asymptote Sectors of integrands vanishing

Analytical results (with surprises) Cold magnetized plasma Condon medium exact roots ultrarelativistic motion weak chirality low frequencies relativistic motion high frequencies

Cold magnetized plasma Analytical results Cold magnetized plasma wave field (VCR) quasistatic field Condon medium – branch points – cuts – poles of Представлены зависимости компонент тензора от частоты и вид комплексной плоскости

Cold magnetized plasma stationary point approach Analytical results Cold magnetized plasma singular vanishing stationary point approach

Numerical results: point charge Cold magnetized plasma

Numerical results: point charge & bunches Cold magnetized plasma

Numerical results: bunches Cold magnetized plasma

Numerical results Condon medium

Numerical results Condon medium

Numerical results Condon medium Gaussian bunch

Thank you for your attention!