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5 Sep 2007: Math. Phys. 20, 19–31 1990.16 Lechtenfeld, O., e-print arXiv:hep-th/0605034.17 Lichnerowicz, A., “Sur l’algèbre de Lie des champs de vecteurs,” Comment. ... Nonlinear Math. Phys. 10, 229–242 2003.20 Merkulov, S. A., “Nijenhuis infinity and

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.

16 Feb 2007: 2ðnÞ. Formula (3.20) follows directly from (1.7) and (3.16). &. Examples. ... References. Anand, C. 1997 Ward’s solitons. Geom. Topol. 1, 9–20. (doi:10.2140/gt.1997.1.9)Bredon, G.

25 May 2007: P. Integrability of the model enables a construction of time dependent solutions by twistor and inverse scatteringmethods [18,20]. ... Math. Phys. 29 (1988) 386–389.[19] R.S. Ward, Integrability of the chiral equations with torsion term, Nonlinearity 1

17 Apr 2007: This lift is thebosonic sector of the lift from N = 2 supergravity in four dimensions to N = 2 supergravity infive dimensions [20, 21]. ... This mistake was corrected more than 20 years later by Jordan and Thiry.

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),.

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.

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}.

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.

11 Apr 2007: when n = 20 and = 0.1.Thus we have two examples of theoretical bounds on the amount of work thatare not useful.