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25 Jan 2007: t per. mis. sion. 20 CHAPTER 4. SOLVING MAXWELL’S EQUATIONS. whereτ0 is the value ofτ on the world-line where the past light cone ofx intersectsthe world line of the

24 Aug 2007: 0 0.2 0.4 0.6 0.80. 10. 20. 30. 40. 50. γ/ρ. ... Ao and D.J. Thouless, Phys. Rev. Lett. 70,2158 (1993). [20] M.

29 Sep 2007: It is sufficiethat the active material is capable to generate the respox x̄i [20]. ... R. SoLondon B 151, 204 (1959), for an actin-myosin system. [20] The model discussed in Ref.

25 Jan 2007: as. Term. 2002. 20. [This. isa. blan. kpage]. Cop. yrig. ht.

25 Jan 2007: Thus, we let. LM Mx ik[σ3, M ] QM. (4.3.8). 20. ... Equation (4.3.10)implies that. M(0)1 =. i. 2Qσ3. (4.3.20). The diagonal part of equation (4.3.18) yields.

19 Oct 2007: right): solid, dashed and dotted lines represent truncation for n1, n2 N , wheren = 10, 20, 40 respectively. ... 20. generalizations, but nothing more. We have. d[0]m,n = c[0]m,n, m, n Z+;.

21 Nov 2007: We see in these tests that thesimplification to BOBYQA provides major gains in efficiency, except in some ofthe n = 20 cases. ... Wecontinue to take n from the set {10, 20, 40, 80, 160, 320} for our numerical tests.

25 Jan 2007: For chargesand currents in a non-polarisable and nonmagnetisable medium, such as the vacuum,these are rE @B@t = 0 (18)r B = 0 (19)r E = 10 (20)rB = ... r j 0 @@t (r E)0 = r j @@t : (26)Here (20) has been used.

7 Aug 2007: 60. -40. -20. 20. 40. Plot of the functionx2. Sin@x2D. Figure 4: The function is singular at points 2πk, k Z{0}.

19 Jun 2007: 3.8 Applications 20. 3.8.1 Vortices and Mirror Symmetry 21. 3.8.2 Swapping Vortices and Electrons 21. ... vortices scattering at right angles [20]. The key point is that the Z2 action in (3.23),.