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  2. D-Branes in Field Theories

    www.damtp.cam.ac.uk/user/tong/talks/dbrane.pdf
    23 Feb 2006: 5. 0. 5. 10. -10-50510. -20 -10 0 10 20. Isozumi, Nitta, Ohashi and Sakai ‘04.
  3. caqcd.dvi

    www.damtp.cam.ac.uk/user/tong/talks/caqcd.pdf
    12 Sep 2006: 5. 10. -10-50510. -20 -10 0 10 20. -10. -5. Figure 3:.
  4. Cambridge NA Report NA2006/01 Joint Diagonalization on the Oblique ...

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2006_01.pdf
    24 Jan 2006: Matrix Anal. Appl. 20 (1998), no. 2, 303–353. [Gab82] D. Gabay, Minimizing a differentiable function over a differential manifold, Journal of Opti-mization Theory and Applications 37 (1982), no. ... Numer. Anal. 20 (1983), 626–637. [TL02] N. T.
  5. Motion of a vortex line near the boundary of ...

    www.damtp.cam.ac.uk/user/ngb23/publications/boundary.pdf
    20 Oct 2006: of Eq. 20 for the uniform flow was found 11 as1 = u1x , y iv1x , y where. ... 0 5 10 15 20. 0.1. 0.2. 0.3. 0.4. 0.5. 0.6.
  6. berloff.dvi

    www.damtp.cam.ac.uk/user/ngb23/publications/warwick.pdf
    7 Sep 2006: complexes. In higher dimensions,domain walls 19 and skyrmions (vortons) 20 have been found. ... 20 -10 0 10 20-20. -10. 0. 10. 20. -20 -10 0 10 20-20.
  7. Numerical approximation of vector-valued highly oscillatory integrals …

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2006_06.pdf
    26 Jul 2006: 25 30 35 40 45 50. 0.050.10.150.20.250.3. Figure 2: The error scaled by ω7/4 of QL[f] with endpoints for nodes and multiplicities both ... 25 30 35 40 45 50. 0.050.10.150.20.250.30.35. Figure 3: The error scaled by ω13/4 of QL[f] with endpoints for
  8. On the linear stability of splitting methods Sergio Blanes1∗ ...

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2006_08.pdf
    2 Sep 2006: λ1(x) = eiΦ(x), λ2(x) = eiΦ(x), (2.21). where Φ(x) is given by (2.20). ... p(x) = cos(x) O(x2n2) as x 0,. i.e. Φ(x) = x O(x2n1) in (2.20).
  9. Paper1.dvi

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2006_05.pdf
    20 Jun 2006: 0.05. 20. 0.1. 0.0. 4 102. 0.025. 1886. 0.075. 0.04. 0.06. ... 20. The method (3.6) cannot be used for approximatingf̂C0 and is less precise for small valuesof n, before the onset of asymptotic behaviour.
  10. N13LBb.dvi

    www.damtp.cam.ac.uk/user/rrh/notes/N13LBb.pdf
    22 May 2006: 2 PARTIAL DIFFERENTIAL EQUATIONS 20. • at x = L apply insulating boundary condition: there is no flux of heat to x > L.Then have Θx(L,t) = 0, t 0: Neumann condition;. • ... 0 1 2 3 4 5x. 0. 5. 10. 15. 20.
  11. DAMTP 2006/NA03 Fast evaluation of polyharmonic splines in three ...

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2006_03.pdf
    31 Aug 2006: The. 20 Fast evaluation of 3D polyharmonic splines. per panel accuracy, and its estimation, are described later. ... 2.20(1)64, 000 3.75(4) 5.31(7) 3.66(0) 1.08(1) 9.06(1).

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