Search

Search Funnelback University

Search powered by Funnelback
31 - 40 of 112 search results for katalk:PC53 24 / |u:www.damtp.cam.ac.uk where 0 match all words and 112 match some words.
  1. Results that match 1 of 2 words

  2. susyqm

    www.damtp.cam.ac.uk/user/tong/susy/susyqm3.pdf
    4 Oct 2023: We can compute the Witten index by simply. summing over the critical points X, just as we did in (1.24).
  3. 10th_Popov_Prize

    www.damtp.cam.ac.uk/user/mjc249/talks/Popov_talk_FoCM_mjc.pdf
    15 Jul 2023: 24/37. 𝐴 𝑚𝑁 modality,𝑚 < 𝑁 , 𝑆 = 𝑦𝑘 𝑘=1𝑅 samples. ... 24] Colbrook, Matthew J. "Computing semigroups with error control." SIAM Journal on Numerical Analysis 60.1 (2022): 396-422.
  4. Microswimmers in vortices: dynamics and trapping

    www.damtp.cam.ac.uk/user/lauga/images/cover_214.pdf
    14 Feb 2023: KaðzÞffiffiffiffiffip2z. rez 1þ4a. 2 18z. þð4a2 1Þð4a2 9Þ. 128z2. ; (24).
  5. Preprint typeset in JHEP style - HYPER VERSION January ...

    www.damtp.cam.ac.uk/user/tong/qhe/one.pdf
    26 Jan 2023: x, y) = n,k(x mE/eB2, y) (1.24). and the energies are now given by. ... 24 –. which obey @z = @̄z̄ = 1 and @z̄ = @̄z = 0.
  6. COMPUTING SPECTRA – ON THE SOLVABILITY COMPLEXITY INDEX HIERARCHYAND…

    www.damtp.cam.ac.uk/research/afha/anders/SCI_FINAL.pdf
    20 Nov 2023: Brown [27–29]) and Toeplitztheory (see A. Böttcher & B. Silberman [24–26]).
  7. J. Fluid Mech. (2017), vol. 828, pp. 33–56. c© ...

    www.damtp.cam.ac.uk/user/drh39/2017_taylor.pdf
    1 Dec 2023: Received 24 February 2017; revised 22 May 2017; accepted 10 July 2017;first published online 30 August 2017).
  8. 4. Continuous Symmetries So far we have focussed almost ...

    www.damtp.cam.ac.uk/user/tong/sft/four.pdf
    14 Jan 2023: 2e20. Zddx. (4.24). The factor of N in front of the first term is what gives us hope because, in the limit. ... Specifically, we send N! 1,. keeping e20N fixed. The path integral (4.24) is then dominated by the minimum.
  9. Vigorous convection in porous media

    www.damtp.cam.ac.uk/user/drh39/2020_hewittreview.pdf
    1 Dec 2023: u = 0. (2.1). In place of the Navier–Stokes equations for an unconfined fluid, in a porous medium the Darcyvelocity u is governed by Darcy’s Law [23,24], which
  10. The mpEDMD Algorithm for Data-Driven Computations of…

    www.damtp.cam.ac.uk/user/mjc249/pdfs/mpEDMD.pdf
    16 Jun 2023: Therefore, its spectral information can be far more complicatedand more difficult to compute than that of a finite matrix [91, 20, 5, 24, 22].
  11. fluids

    www.damtp.cam.ac.uk/user/tong/fluids/fluids1.pdf
    9 May 2023: V. d3x0J(x0). |x x0|. – 24 –. If we subsequently take the curl of this equation, then we get an expression for the.

Refine your results

Search history

Recently clicked results

Recently clicked results

Your click history is empty.

Recent searches

Your search history is empty.