Radiation from charged particles

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Presentation transcript:

Radiation from charged particles PHY 712 Electrodynamics 9-9:50 AM MWF Olin 105 Plan for Lecture 29: Finish reading Chap. 14 – Radiation from charged particles Review of synchrotron radiation Free electron laser Thompson and Compton scattering 04/5/2019 PHY 712 Spring 2019 -- Lecture 29

04/5/2019 PHY 712 Spring 2019 -- Lecture 29

04/5/2019 PHY 712 Spring 2019 -- Lecture 29

Advice about remaining topics to cover Cherenkov radiation Electrodynamics of superconductivity Radiation from collisions of charged particles Optical properties of materials 04/5/2019 PHY 712 Spring 2019 -- Lecture 29

Spectral composition of electromagnetic radiation -- continued 04/5/2019 PHY 712 Spring 2019 -- Lecture 29

y z x b . r q Top view: y x r 04/5/2019 PHY 712 Spring 2019 -- Lecture 29

y z x b . r q 04/5/2019 PHY 712 Spring 2019 -- Lecture 29

y z x b . r q 04/5/2019 PHY 712 Spring 2019 -- Lecture 29

04/5/2019 PHY 712 Spring 2019 -- Lecture 29

of discrete multiples of v/r. Evaluation of integrals representing distant charged particles moving in a circular trajectory such that the spectrum represents a superposition of light generated over many complete circles. In this case, there is an interference effect which results in the spectrum consisting of discrete multiples of v/r. 04/5/2019 PHY 712 Spring 2019 -- Lecture 29

Useful identity involving Bessel functions 04/5/2019 PHY 712 Spring 2019 -- Lecture 29

Astronomical synchrotron radiation -- continued: 04/5/2019 PHY 712 Spring 2019 -- Lecture 29

Astronomical synchrotron radiation -- continued: In both of the expressions, the sum over m includes both negative and positive values. However, only the positive values of w and therefore positive values of m are of interest. Using the identity: the result becomes: These results were derived by Julian Schwinger (Phys. Rev. 75, 1912-1925 (1949)). The discrete case is similar to the result quoted in Problem 14.15 in Jackson's text. 04/5/2019 PHY 712 Spring 2019 -- Lecture 29

04/03/2019 PHY 712 Spring 2019 -- Lecture 28

04/03/2019 PHY 712 Spring 2019 -- Lecture 28

Plots of the intensity function for synchrotron radiation gq=0 gq=0.5 gq=1 gq=1 gq=0.5 w/wc w/wc 04/5/2019 PHY 712 Spring 2019 -- Lecture 29

Plots of the intensity function for synchrotron radiation w/wc=1 gq 04/5/2019 PHY 712 Spring 2019 -- Lecture 29

Synchrotron facilities worldwide https://lightsources.org/ 04/5/2019 PHY 712 Spring 2019 -- Lecture 29

Free electron laser Reference: 04/5/2019 PHY 712 Spring 2019 -- Lecture 29

04/5/2019 PHY 712 Spring 2019 -- Lecture 29

04/5/2019 PHY 712 Spring 2019 -- Lecture 29

04/5/2019 PHY 712 Spring 2019 -- Lecture 29

Electron emission in periodic magnet 04/5/2019 PHY 712 Spring 2019 -- Lecture 29

Spectral output for FEL at Jefferson Lab (in Virginia) 04/5/2019 PHY 712 Spring 2019 -- Lecture 29

04/5/2019 PHY 712 Spring 2019 -- Lecture 29

Some details of scattering of electromagnetic waves incident on a particle of charge q and mass mq k0 q e2 e0 f e1 04/5/2019 PHY 712 Spring 2019 -- Lecture 29

Thompson scattering – non relativistic approximation 04/5/2019 PHY 712 Spring 2019 -- Lecture 29

Thompson scattering – non relativistic approximation -- continued k0 q e2 e0 f e1 04/5/2019 PHY 712 Spring 2019 -- Lecture 29

Thompson scattering – non relativistic approximation -- continued Scattered light may be polarized parallel to incident field or polarized with an angle q so that the time and polarization averaged cross section is given by: This formula is appropriate in the X-ray scattering of electrons or soft g-ray scattering of protons 04/5/2019 PHY 712 Spring 2019 -- Lecture 29

Thompson scattering – relativistic and quantum modifications pq incident photon a p q p’ scattered photon 04/08/2013 04/5/2019 PHY 712 Spring 2019 -- Lecture 29 30

Thompson scattering – relativistic and quantum modifications pq incident photon a p q p’ scattered photon 04/5/2019 PHY 712 Spring 2019 -- Lecture 29