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13 Jun 2008: On the basis of 24 successful projects over the initial three years of NaTII, the estimated budget is £7 million.

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.

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.

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.

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

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).

3 Jul 2008: 1 |φn |2)p2 d x (24). and1. 4π. jφp(x)d x = limn1. ... Ann. Math. 113, 1–24 (1981)22. Schoen, R., Uhlenbeck, K.: Boundary regularity and the Dirichlet problem for harmonic maps.

18 Mar 2008: eA00fA D 0; (24)eA10fA D 0: (25). Anti-self-dual conformal structures in neutral signature 123. ... 4Other terminology includes neutral hyper-Kähler [28] and hyper-para-Kähler [24]. Anti-self-dual conformal structures in neutral signature 127.

17 Jan 2008: 24. 2.1.2 The Arc Length. 25. 2.1.3 The Tangent. 26. 2.1.4 The Osculating Plane. ... Mathematical Tripos: IA Vector Calculus 16 c S.J.Cowley@damtp.cam.ac.uk, Lent 2000. differentiability (1.24):3.

30 Sep 2008: with width 1/σ (See figure (13)) We will now evaluate the resulting wave-function bysubstituting (24) for A in (23),. ... ψ|2U. 0x0(t). Figure 24: Initial state of wavepacket. x. |ψ|2U. 0.

3 Jul 2008: self-dual structure provides a useful way of rewriting this formula as in (2.24), in terms. ... behaviour of critical points in the λ limit, starting with [4]; see [24] and references.

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

3 Jul 2008: For the first time, the asymptotics of type (1.2) were established by Soffer and Weinstein[24, 25] (see also [20]) for nonlinear U(1)-invariant Schrödinger equation with small initial ... c(ν)(t s)1/2(‖η(s)‖2Lβ ρ‖η(s)‖Lβ. ), 0 < t s < ν.

6 May 2008: L. (3.24). By taking logarithms of both sides of expression (3.23), we find the inequality.

1 Aug 2008: µ4(ω) =25I0(τ). 2. ωΘ. [2]0 (ω). 8. ω2Φ. [2]0 (ω). 24.

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

5 Dec 2008: This equation determines λ as a function of α. 24. Cop.

10 Apr 2008: Re λm (mπ)2. ω4. 2(mπ)2 5/24(mπ)4. ω6+ O(ω8), (3.1). Im λm 2.

1 Apr 2008: Multiple Jets as PV Staircases: The Phillips Effect and the Resilience ofEddy-Transport Barriers. D. G. DRITSCHELMathematical Institute, University of St. Andrews, St. Andrews, United Kingdom. M. E. MCINTYRECentre for Atmospheric Science, Department

23 Sep 2008: f• -. •'(y, z) (24). and the mean meridional and vertical velocities •,fv satisfy a zonally symmetric mass-conservation equation of the form. ... A more accurate 92 - version of (26), based on a more accurate version of (24), is presented by P.

29 Jan 2008: 502, Campus Universitaire, Orsay, F-91405, France. B. PerrinLaboratoire Pierre Aigrain, UMR 8551, CNRS, Ecole Normale Supérieure, Département de Physique,24 rue Lhomond, 75231 Paris Cedex 05, France.

3 Jul 2008: as2@cam.ac.uk. eived 9 March 2007epted 24 July 2007 2753 This journal is q 2007 The Royal Society.

29 Jan 2008: DAMTP 2008/NA03. On nonlinear optimization since 19591. M.J.D. Powell. Abstract: This view of the development of algorithms for nonlinear optimiza-tion is based on the research that has been of particular interest to the authorsince 1959, including

8 Apr 2008: 23. 2.2.4 N = 1 Supersymmetry Representations. 24. 2.2.5 Massless Supermultiplet. ... i.e. as predicted 16 = 24 states in total. Notice that these multplets are much larger than the.

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

27 Jan 2008: A Theoretical Framework forBackward Error Analysis on Manifolds. Anders C. Hansen. January 25, 2008. DAMTP, Centre for Mathematical SciencesUniversity of Cambridge, Wilberforce Rd, Cambridge CB3 0WA. e-mail: A.Hansen@damtp.cam.ac.uk, Ph: 44 1223

3 Oct 2008: 24. the three coordinate directions. They span a parallelepiped of volume.