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6 Oct 2020: sions in solids. Detailed balance. Maxwell, Bose-. Einstein and Fermi-Dirac distributions.

8 Mar 2012: Articles of this kind in principle have a role, in cases of genuine roguery (the late Robert Maxwell comes to mind as an example of someone who might deserve such treatment).

7 Jan 2019: αβ ,. where Fµν = µAν νAµ, one obtains two Maxwell’s equations for a freeelectromagnetic field from the Euler-Lagrange equations:. ... µFµα = 0. These are just the (inhomogeneous) Maxwell equations:. E = 0 , B = ε0µ0E.

7 Jan 2019: αβ ,. where Fµν = µAν νAµ, leads to two of Maxwell equations for a freeelectromagnetic field.

7 Jan 2019: which are the inhomogeneous Maxwell equations.(c) A gauge transformation is performed by adding the derivative of a scalar.

29 Sep 2016: Maxwell equations (4)-(7) and shown in Fig 2. The valueof the surface energy σsn is given by the extra contributionto the Gibbs potential G.

7 Jan 2019: 4 The ‘Maxwell-Chern-Simons’ Lagrangian is. LMCS = 1. 4FµνF. µν gϵµνλAµνAλ.

20 Jan 2016: αβ ,. where Fµν = µAν νAµ, leads to two of Maxwell equations for a freeelectromagnetic field.

8 Jan 2009: which are the inhomogeneous Maxwell equations.(c) A gauge transformation is performed by adding the derivative of a scalar.

24 Jan 2011: 4 The ‘Maxwell-Chern-Simons’ Lagrangian is. LMCS = 1. 4FµνF. µν gϵµνλAµνAλ.

19 Oct 2009: 5The electric field E and magnetic field B of Maxwell’s equations contain only “physical”degrees of freedom, in the sense that every mathematical degree of freedom in an electromag-netic

26 Feb 2018: Figure 1: A cavity. We solve the (sourceless) Maxwell’s equations withinthe cavity subject to the boundary condition that theelectric field must vanish at the cavity walls:.

31 Dec 2017: follow Maxwell's equations and the full. o(2J and. Lagrangian. l: f mc2_ } - vc dt - - --. particles. ( l: J e. A dx. ]. 1.1 changes. , ' ,. is. ,. ,. 0 : ,! ''.•. The Hamiltonian is interesting ... 2. c at. and similarly for all the other Maxwell

28 Nov 2023: C., Manou, I., Maxwell, G., Prieto, P., Roggeband, R., Sobanski, T., Schütte, K., Worth,.

26 Jan 2012: regions ofdensity 1=2 and 1 at long time scales, as demonstratedin the inset by a Maxwell construction for the energy of aphase separated system composed of the adjacent stablephases.

10 Nov 2013: Lecture I 1. Lecture I: Collective Excitations: From Particles to Fields. Free Scalar Field Theory: Phonons. The aim of this course is to develop the machinery to explore the properties of quantumsystems with very large or infinite numbers of

4 Jan 2023: 2Jβ is the effective magnetic field. Using Maxwell’s relation. (µ. V. ).

5 Feb 2019: Ab Initio Electron Energy Loss. Spectroscopy. A dissertation submitted for the degree of Doctor of. Philosophy at the University of Cambridge. Chris J. Pickard. Christ's College, Cambridge. September 1997. Preface. This dissertation describes work