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91 - 100 of 132 search results for katalk:PC53 24 / |u:www.damtp.cam.ac.uk where 0 match all words and 132 match some words.

  1. Results that match 1 of 2 words

  2. J. Fluid Mech. (2018), vol. 837, pp. 520–545. c� ...

    www.damtp.cam.ac.uk/user/jneufeld/pubfiles/Nijjer-2018a.pdf
    6 May 2019: 44. 40C. 08:0. 1:4. 07. DD. D 2. 01. 834. 24. ... 01. 834. 24. 4. 530 J. S. Nijjer, D. R. Hewitt and J.

  3. The N-flagella problem: elastohydrodynamic motility transition of…

    www.damtp.cam.ac.uk/user/lauga/papers/161.pdf
    27 May 2019: Despite these variations, acoherent flagellar bundle is expected to be maintained generically by long-range hydrodynamicinteractions [24,25]. ... 2.24). For a symmetric configuration such that (N. i=1 ω̃(i)t Ri) ez = 0, only the first term of Mprop.

  4. EuroStrings2015.key

    www.damtp.cam.ac.uk/research/hep/files/conferences/EurostringTalks/Dabholkar.pdf
    6 Feb 2019: 12 -208 208.455 53252. 15 513 512.958 192401. 23. ATISH DABHOLKAR QUANTUM ENTROPY OF BLACK HOLES 24. •

  5. 9 Perturbation Theory II: Time Dependent Case In this ...

    www.damtp.cam.ac.uk/user/dbs26/PQM/chap9.pdf
    4 Dec 2019: t0〈k||m〉eiωkmt′ dt′ = km. Ek Em(1 eiωkmt. ), (9.24). where km = 〈k||m〉 and ωkm = (Ek Em)/. ... k|†|m〉(ωkm ω). [ei(ωkmω)t 1. ]. (9.32). This is very similar to our result (9.24), with the time–dependence of the perturbation.

  6. D6 R4

    www.damtp.cam.ac.uk/research/hep/files/conferences/EurostringTalks/Vanhove.pdf
    6 Feb 2019: Pierre Vanhove (IPhT & IHES) D6 R4 Cambridge March 2015 24 / 37.

  7. Geophys. J. Int. (2019) 218, 247–267 doi: 10.1093/gji/ggz139Advance…

    www.damtp.cam.ac.uk/user/jneufeld/pubfiles/Ball-2019.pdf
    22 Jul 2019: ic.oup.com/gji/article-abstract/218/1/247/5382046 by U. niversity of Cam. bridge user on 24 June 2019. ... bridge user on 24 June 2019. Evolution of thin-skinned fold-thrust belts 257.

  8. Bootstrapping the (2,0) theories in six dimensions

    www.damtp.cam.ac.uk/research/hep/files/conferences/EurostringTalks/VanRees.pdf
    6 Feb 2019: O1(x1)O2(x2)O3(x3)O4(x4)〉. =k. λ k12λk. 34@. @k=p. λ p13λp. 24. @. @p.

  9. Universal optimal geometry of minimal phoretic pumps

    www.damtp.cam.ac.uk/user/lauga/papers/165.pdf
    20 Oct 2019: 339,. 936–940 (2013). 24. Duan, W. et al. Synthetic nano- and micromachines in analytical chemistry: sensing, migration, capture, delivery and separation.

  10. On reconstructions from measurements with binary functions Robert…

    www.damtp.cam.ac.uk/research/afha/anders/Matheon_Springer_Final.pdf
    10 Apr 2019: Moreover, we have for the transform, that it is linear:. W {af(x) bg(x)} = aW {f(x)} bW {g(x)} a,b R, f,g L2([0, 1]d), ... 5.1 Classical compressed sensing. Compressed sensing was introduced by Candès, Romberg & Tao (19) and Donoho (24)and is

  11. Preprint typeset in JHEP style - HYPER VERSION Lent ...

    www.damtp.cam.ac.uk/user/tong/aqm/aqmone.pdf
    19 Jul 2019: qg = 2n with n 2 Z (1.24). This is the famous Dirac quantisation condition. ... qg = 2n with n 2 Z. This, of course, is the Dirac quantisation condition (1.24).

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