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  2. PowerPoint Presentation

    www.damtp.cam.ac.uk/user/pvl/GOOSE/cox.pdf
    20 Sep 2009: Employment has fallen 24,000 in the last quarter. Unemployment now 6.5 per cent (4.6 per cent a year ago).
  3. Slide 1

    www.damtp.cam.ac.uk/user/pvl/GOOSE/cannard.pdf
    20 Sep 2009: you will help save paper. Responses needed by Tue 24 November 2009.
  4. 26 Apr 2009: 24) D. Bruss, N.Datta, A. Ekert, L.C. Kwek and C. Macchiavello, Multipartite entangle-.
  5. Dynamics of quantum vortices in a toroidal trap Peter ...

    www.damtp.cam.ac.uk/user/ngb23/publications/toroidal09.pdf
    3 Sep 2009: R1. 2r0R2. 2. R12. r0 R1 , 24. where a sign has been added to indicate the circulationof the vortex.
  6. PhysicaD238 (2009)1289–1298 Contents lists available at ScienceDirect …

    www.damtp.cam.ac.uk/user/ngb23/publications/physicaDintro.pdf
    3 Sep 2009: Despite the numerous results already obtained in thefield, therearestillmanyopenproblemsandtherehasbeenaburstof new experimental results in the last few years [24,25,29,31]. ... and also between solitons [24,25,39] still clearly have a lot
  7. IOP PUBLISHING FLUID DYNAMICS RESEARCH Fluid Dyn. Res. 41 ...

    www.damtp.cam.ac.uk/user/ngb23/publications/fdr09.pdf
    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. 29 Jan 2009: 24. Recall Section 1.6: A is not unique, because we can transform the vector potential according to.
  9. 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).
  10. Extrinsic1b.dvi

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2009_09.pdf
    1 Dec 2009: 3.24). The corresponding result is the following. Theorem 2 Let f(y) be constant, then we have θ0 = 0, θ1 = ̺ and. ... θs = (s 1)̺, s 2.Proof We shall use formula (3.24) and proceed along the lines of theproof of Theorem.
  11. DAMTP 2009/NA06 The BOBYQA algorithm for bound constrained…

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2009_06.pdf
    12 Aug 2009: 12α2 (1 α)2 ‖y. j xk‖4, αR, (4.24). the last line being due to the positive semi-definiteness of =ZZT.

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