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  1. Results that match 1 of 2 words

  2. 0405FINAL.qxd

    https://api.newton.ac.uk/website/v0/annual-reports/2004/2005
    Secretary) Deputy Director, Newton InstituteProfessor PT Johnstone St John’s CollegeProfessor Sir John Kingman FRS Director, Newton InstituteProfessor PV Landshoff (Chairman) General Board Professor TJ Pedley FRS Head of Department, DAMTPProfessor
  3. Computational Challenges in Partial Differential Equations

    https://api.newton.ac.uk/website/v0/events/cpd/reports/scientific-report
    dissipation properties of these methods. P Houston and TJ Barth developed a new post-.
  4. One-dimensional scaling limits in a planar Laplacian random growth ...

    https://api.newton.ac.uk/website/v0/events/preprints/INI1410
    ds. ). We next obtain bounds on Hj(t), under the assumption that t 6 Tj, where. ... 25|u0t (z0)|and. |δjt | 64|u0t (z0)eiξ. 0T t 1|. 25. for all t 6 Tj.
  5. shub.dvi

    https://api.newton.ac.uk/website/v0/events/preprints/NI00028
    For i < j setf[i;j = f[j;i = 1 ti=tj1 ti=tj = 12titj 2t2it2j 2t3it3j : : : 2LThis fun tion also satises the ondition of Proposition. ... Indeed, if for i < j < k we set a = ti=tj,b = tj=tk, then the identity we should verify redu es to the orre t
  6. A polynomial bound on the diameter of the transportation ...

    https://api.newton.ac.uk/website/v0/events/preprints/NI02033
    11] Tj.C. Koopmans, Optimum utilization of the transportation system, inD.H. Leavens (ed.), The Econometric Society Meeting, Washington DC,1947, 1948, 136–146.
  7. A Quadratic Bound on the Diameter of the Transportation ...

    https://api.newton.ac.uk/website/v0/events/preprints/NI02044
    11] Tj. C. Koopmans, Optimum utilization of the transportation system, in D.
  8. 1 AC losses in type-II superconductors induced bynonuniform…

    https://api.newton.ac.uk/website/v0/events/preprints/NI03053
    Of course, the same inequality may be written as(G tJ 1µ0 tAe, Φ J. ) ... It is easy to see that T0. J G tJ ddt =. T0. d. dt. {12. J G J d. }dt = 0.
  9. EFFECTIVE SIMULATION OF A MACROSCOPIC MODEL FOR STATIONARY…

    https://api.newton.ac.uk/website/v0/events/preprints/NI03070
    T := (b[j,1], b[j,2])T |Tj|(mhT z) z. Tj. f dx;(. M11jj M12jj. ... substituted by m(n)h. (iv) Mark an element Tj T (n) provided ηj θ max1kN.
  10. EFFECTIVE RELAXATION FOR MICROSTRUCTURE SIMULATIONS:ALGORITHMS AND…

    https://api.newton.ac.uk/website/v0/events/preprints/NI03087
    of. Algorithm 1 (Adaptive Algorithm). Input is an initial triangulation T = Tj for j = 0.(a) Solve Problem (3.2) (with a Newton-Raphson or Quasi-Newton method).(b) Compute indicators ... EFFECTIVE RELAXATION FOR MICROSTRUCTURE SIMULATIONS 21. (i) Choose
  11. On the Moments of Tracesof Matrices of Classical Groups ...

    https://api.newton.ac.uk/website/v0/events/preprints/NI04015
    On the Moments of Tracesof Matrices of Classical Groups. L. Pastur 1,2, and V. Vasilchuk 2. 1 University Paris 7, Paris, France2 Institute for Low Temperature Physics, Kharkov, Ukraine. AbstractWe consider random matrices, belonging to the groups U(n

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