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7 May 2008: 24] for an analogous study of the one component sys-tem). Acknowledgments. ... Low Temp. Phys. 146, 31. (2007).[24] A. Picozzi, Optics Express, 15, 9063 (2007).

26 Feb 2008: Mercury has e 0.2 and Pluto has e 0.24. All the other planets have e < 0.1, so the difference betweenthe minor and major axes of their orbits is

18 Mar 2008: We omit the lemma and state the theorem. Theorem 4.3 Define the quadrature rule QM [f ] with points and weights givenby (24). ... Comp., 76:1341–1356, 2007. [24] R. Wong. Asymptotic approximations of integrals. Academic Press, 1989.

25 Sep 2008: For = (ts t) 1 it follows from (3) and (23)that the dimensional blowing velocity has magnitudev̂b = O(U Re12 74 ) : (24)This blowing velocity causes a perturbation to the inviscid ... the continuity equation it follows thatthe perturbation velocity in

31 Jul 2008: 9.3.9]:. u0(t) = 1, u1(t) =3t 5t3. 24, u2(t) =. 81t2 462t4 385t61152. , ... 9.6.24]. Kν (νz) =1. 2. eνφ(v) dv, φ(v) = z cosh v v.

3 Jun 2008: Consider a single first order PDE. F(x1,. ,xn,u,. u. x1,. ,. u. xn. )= 0. (4.1). 24. This PDE defines a co–dimension one manifold M J1(Rn, R) of

29 Jan 2008: B. PerrinLaboratoire Pierre Aigrain, UMR 8551, CNRS, Ecole Normale Supérieure,Département de Physique, 24 rue Lhomond, 75231 Paris Cedex 05, France. ... Combining Eqs. 21, 24, and 25 leads to the nonlin-ear diffusion equation satisfied by the local

26 Feb 2008: V 2X′ 2 V 2Y ′ 2 V Y ′. 24.

1 Jul 2008: The Riemann–Hilbert factorization problem underlies this approachto integrability: it appears in classical solution generating techniques such as dressingtransformations [18], as well as in the twistor treatment of ASDYM [24]. ... Math. Phys. 7

11 Aug 2008: 24,25]. By studying the stability of these steady-state solutions, one finds that with homogeneous pumpingthese solutions become unstable to breaking of rotationalsymmetry. ... 24] M. A. Porras, A. Parola, D. Faccio, A. Dubietis, and P.