Search

5 Dec 2008: Using Cartesian coordi-nates, calculate the electric current density J given by the steady Maxwell equation B = µ0J.

13 Mar 2008: µ0BkBk. )). Using Maxwell’s equations, show that. t(ǫ0E B) = M ρE J B.

3 Jul 2008: The solitarywaves were introduced by Schrödinger for the quantum electron coupled to the Maxwell field,[23]. ... He identified the solitary waves with the quantum stationary states. The asymptoticsof type (1.2) for the coupled U(1)-invariant

3 Oct 2008: Electromagnetic waves. Maxwell’s equations for the electromagneticfield in a vacuum:. E = 0. ... Eliminate E:. 2B. t2= E. t= 1. µ0ǫ0 ( B). Now use the identity ( B) = ( B) 2B and Maxwell’sequation B = 0 to obtain the (vector) wave equation.

3 Jul 2008: ii) Example 2: the Yang–Mills–Higgs equations. Yang–Mills theory is a nonlinear variant of Maxwell’s electromagnetism inwhich the field strength is described by a two-form Fmndx.

3 Jul 2008: Adiabatic limit and the slow motion of vortices in a. Chern-Simons-Schroedinger system. Sophia Demoulini and David StuartCentre for Mathematical Sciences, Wilberforce Road, Cambridge, CB3 OWB, England. email:sd290@cam.ac.uk, dmas2@cam.ac.uk.

8 Apr 2008: Supersymmetry and Extra. Dimensions. Lectures by: Fernando Quevedo, Notes by: Oliver Schlotterer. April 8, 2008. 2. Contents. 1 Physical Motivation for Supersymmetry and Extra Dimensions 7. 1.1 Basic Theory: QFT. 7. 1.2 Basic Principle: Symmetry. 8.

24 Apr 2008: Preprint typeset in JHEP style - PAPER VERSION June 2005. TASI Lectures on SolitonsInstantons, Monopoles, Vortices and Kinks. David Tong. Department of Applied Mathematics and Theoretical Physics,. Centre for Mathematical Sciences,. Wilberforce Road,

17 Jan 2008: Mathematical Tripos: IA Vector Calculus. Contents. 0 Introduction i. 0.1 Schedule. i. 0.2 Lectures. i. 0.3 Printed Notes. ii. 0.4 Examples Sheets. iii. 0.5 Previous Comments, Comments on Comments and Style of Lectures. iii. 0.6 Books. iv. 0.7