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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).

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.

24 Aug 2009: http://journals.cambridge.org Downloaded: 24 Aug 2009 IP address: 131.111.16.227. J. Fluid Mech. ... http://journals.cambridge.org Downloaded: 24 Aug 2009 IP address: 131.111.16.227. 804 E. J.

10 Nov 2009: Received 8 June 2009; accepted 3 August 2009; published online 24 September 2009.

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

14 Jul 2009: http://journals.cambridge.org Downloaded: 14 Jul 2009 IP address: 131.111.16.227. J. Fluid Mech. (1996), t d 308, p p. 255-288 Copyright @ 1996 Cambridge University Press. 255. Computer simulations of polymer chain relaxation via Brownian motion. By

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.

8 Jul 2009: 1–24 of the Collected Papers, Vol. 3, M. Y. Hussaini, Ed., Oxford.

13 Jul 2009: ARTICLES. Hydrodynamic interactions in deep bed filtrationClaude GhidagliaLaboratoire de Physique et Mecanique des Milieux Hetérogènes, URA 857 au CNRS, ESPCI, 10 rueVauquelin, 75231 Paris Cedex 05, France. Lucilla de ArcangelisLaboratoire de

14 Jul 2009: Quite clearly the time-step 6 t = 0.03, with the large random displacement (2D6t)'l2 = 0.24, smears out the details which are to be resolved.