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16 Jan 2009: n E|. =1. ǫ0σ (23). nE|. = 0. (24). b). Let S carry current density s per unit length (charge crossing unit length in S in unittime).

29 Jan 2009: 24. Recall Section 1.6: A is not unique, because we can transform the vector potential according to.

26 Apr 2009: 24) D. Bruss, N.Datta, A. Ekert, L.C. Kwek and C. Macchiavello, Multipartite entangle-.

15 Oct 2009: 2ψ22) 2me2N Φ21. (e2N 1)2. 2me2Nψ22 4. rΦ1ψ2. = O(1),. (1.24). ... To see this, observe that by (1.24) and the preceding remarks, the equationF(l,Q,N, Φ1,ψ2; 0) = 0 amounts to.

17 Sep 2009: It has been developed over the last30 years by the Oxford school of Penrose and Atiyah with the crucial early input from Ward[24, 25] and Hitchin [10, 11] and further ... Sächs. Akad. Wiss. Leipzig, Maths. Nat. Kl 69 262–77[24] Ward R S 1977 On

13 Jul 2009: Lipscombe, R. Kennings and M.M. Denn, J. Non-Newtonian Fluid Mech., 24 (1987) 85 [l]). ... References. 1 G.G. Lipscomb, R. Keunings and M.M. Denn, J. Non-Newtonian Fluid Mech., 24 (1987) 85-96.

27 Jul 2009: 4.25)We now consider the reduction of the system (4.23),(4.24). Theorem 1.1 arises as acorollary of Proposition 4.2. ... to a coupled system whichincludes the Z3 two dimensional Toda chain [24] as a special case.

30 Aug 2009: 2007) 24–26% 40%(Ridgwell and Hargreaves 2007) 34%(Montenegro et al. 2007) 52%. ... Ambio 24(6):376–378Torn MS, Harte J (2006) Missing feedbacks, asymmetric uncertainties, and the underestimation of future.

31 Jul 2009: www.sciencemag.org SCIENCE VOL 325 24 JULY 2009 489. REPORTS. on. July. ... 24 JULY 2009 VOL 325 SCIENCE www.sciencemag.org490. REPORTS. on. July. 24,.

3 Sep 2009: V|ψ|2 dx = ψ2u v, (24). where v =. V dx, and by ψ the wavefunction of the bulk: ψ ψ as r. ... For thequartic term in the expression for the energy, we write using equation (24).

16 Oct 2009: An estimate of the hydrodynamic coupling between twoidealized flagella [24] is est ’ rRL. ... E.Goldstein, Science 325, 487 (2009). [24] T. Niedermayer, B. Eckhardt, and P.

15 Oct 2009: Theorem 8 ([24]) If the nonlinearity satisfies the conditions given in 1.3.2 then (POS) is true. ... 24). The stabilityis in the same sense as in the previous theorem, see [17] for full details.

10 Jul 2009: For the same trial as in Fig. 5, this constantB is found to be20.90 and 24.29 for the large andsmall angle sides, respectively.

31 Jul 2009: SZAN-IAWSKI, A. 1972 Arch. Mech. 24, 555. TANNER, R. I. 1971 J.

8 Jul 2009: B. PerrinLaboratoire Pierre Aigrain, UMR 8551, Ecole Normale Supérieure, Département de Physique,24 rue Lhomond, 75231 Paris Cedex, 05, France. ... Rev.Fluid Mech. 24, 21 s1992d. 12F. Viana, R. Pardo, R. Yanez, and J.

14 Jul 2009: 0.24 1. 0.18. (T 0.12. 0.06. 0 a. FIGURE 2. The growth rate 0 = aci as a function of wavenumber CI for the varicose mode of a ... The dashed curves are contours of pressure. 0.24. 0.18. 0 0.12.

10 Jul 2009: The displacements xn as a function of position along theline, n, at different times t = 13.5, 24.5, 35.2, and 45.7. ... The different symbols are different times: , t = 13.5; , t = 24.5; , t = 35.2; ,t = 45.7.

13 Jul 2009: Denn, J. Non-Newtonian Fluid Mech., 24 (1987). 85-96. 6 P.J. Coates, R.C.

10 Jul 2009: 1 O f 11/3! (24). Figure 3 shows the settling velocity for a simple cubic arrayspherical particles as a function off 1/3. ... It can be seen that thenumerical results, obtained by considering the finite size ofparticles, yield close agreement with the

8 Jul 2009: B. PerrinLaboratoire Pierre Aigrain, UMR 8551, CNRS, Ecole Normale Supérieure, Département de Physique,24 rue Lhomond, 75231 Paris Cedex 05, France.