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19 Nov 2007: 0.2. 0.0. -20 -10 0 10 20x/t0.5. 25 s. 75 s. ... 0.774t 1.83 20 < t < 25. 0.750t 2.82 90 < t < 100.

23 Apr 2007: If slaves consume food of 1500 Cal day1, 10% of which is available for useful work,how many slaves would be required to do the work over 20 years? ... Over 10. 9 years, a gas would escape ifits average thermal velocity exceeded 20% of the escape velocity.

30 Mar 2007: 10-50510. -20 -10 0 10 20. Isozumi, Nitta, Ohashi and Sakai ‘04.

10 Oct 2007: L = 1. 4FµνF. µν 1. 2m2CµC. µ (20). where Fµν = µCν νCµ.

25 Jan 2007: Aθφ. ). ,1. r. (. 1. sinθ. Arφ. r(rAφ). ). ,. 1. r. (. r(rAθ). Arθ. ) ) (20). 2ψ =1. r2.

21 Jun 2007: L = t wx λy ,(1.2)M = y ux λx. This should be contrasted with Lax pairs for othdispersionless integrable systems[1,10,13,14,20,23which contain derivatives ... Phys. 44 (9) (2003) 4134.[20] K. Takasaki, T. Takebe, Rev. Math.

19 Oct 2007: Ep =. |p |2 m2 (1.20). where we take the ve square root.

30 Mar 2007: 20 40 60 80 100n. 0.002. 0.004. 0.006. 0.008. 20 40 60 80 100n. ... Otherwise,f(1) fn(1) = O. (n1. ). 6. 20 40 60 80 100n.

24 Jun 2007: U P(T U ) ΘZpoint O(1) real line. geodesic point. Dunajski (DAMTP, Cambridge) ASD in ( ) 27 March 2007 20 / 26.

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.

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.

27 Jul 2007: As special cases of (1.3) we recover some examples of[20], where neutral metrics were related to second order ODEs.

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+;.

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

27 Nov 2007: For large n. anan1. ' 2kαn,. 20. and f behaves like exp (2kαρ) = exp (2kr) (so Ψ is not normalizable). ... If a state vector is. |Ψ〉 =. n. cn|Ψn〉, (6.20). where |Ψn〉s are eigen-vectors of  ( i.e, Â|Ψn〉 = an|Ψn〉), then a

15 Feb 2007: Thus, methods really ‘takeoff’ only for fairly large n̄ – for example, the errors ofQ[0,0][20,20],1,3,3 and Q. ... 0,0][20,20],1,2,4 are. 1.186709 and1.294113 – the latter is fairly respectable.Indeed, a significant downside of our approach is

19 Jun 2007: 1.4.2 Constructing the Solutions 20. 1.4.3 Non-Commutative Instantons 24. 1.4.4 Examples of Instanton Moduli Spaces 25. ... original ones, allowing us to define three matrices Ji,. η̄iµν δβAν = (Ji)αβ [δαAµ] (1.20).

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

21 Jun 2007: Math. Phys. 20, 1938. Proc. R. Soc. Lond. A (2002). 1222 M.

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.

25 Jan 2007: 196.5 Further Examples. 20. 6.5.1 The Schwarzschild Metric. 206.5.2 The k = 0 Robertson-Walker Metric. ... d2x. dt2= g(x, t), (19). d2x̃. dt2= g(x N) (20). and sod2N.

6 Nov 2007: which is an example of the behaviour quoted above (20) for G(r). ... 5 LANDAU-GINSBURG THEORY AND MEAN FIELD THEORY 20. A4M3 a2|T Tc|M h , (32).

5 Dec 2007: 4e4,1 = : W A , B , ) , (2.20). ... where. Thus, recalling that A(?, p) = cos9, we see that (2.20) is replaced by (2.36).

13 Apr 2007: It is obvious from the definition that c(E,F) = c(F,E). 20.

2 Nov 2007: Î ¿Ë 2 %Îqü ]ýÁ¢£ &ªU¤X%6: cyÃyw¤¢f¤R«y£&%y6µ¢U¤R XäCO Ë ÄkØyÎ ßß Ë Î),-ÙË 6 2 /. ο 6 20. 2 þ 6 UD%¢ þ1. U¢ Ôu£. i ... 0 20 40 60 80. 0. 5. 10. 15. = 1 >FG A - _ 8 G A}EÃ_ù?AÜJ #G %& jÆA ʤCn%ÇË_ð Ä