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1 - 10 of 13 search results for KA :PC53 |u:www.damtp.cam.ac.uk where 0 match all words and 13 match some words.

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  2. DOI 10.1140/epje/i2015-15007-6 Regular Article Eur. Phys. J. E (2015) …

    www.damtp.cam.ac.uk/user/lauga/papers/104.pdf
    14 Nov 2019: n c = 1 Da c. (45). Here the Damköhler number Da = Ka/κ is a measureof the relative magnitude of reaction and diffusion.

  3. Bayesian Inverse ProblemsLecture notes, Lent term 2019 University of…

    www.damtp.cam.ac.uk/research/cia/files/teaching/Inverse_Problems_Lent_2018/19y_01m_16d_LectureNotes.pdf
    6 Nov 2019: 0. a(ti s)u(s)ds kj=1. 1. ka(ti sj)u(sj) =. kj=1. aijuj,. where we have denoted sj =j1k1 , uj = u(sj) and aij =. 1ka(ti

  4. 15632687789062 1..20

    www.damtp.cam.ac.uk/user/lauga/papers/164.pdf
    20 Oct 2019: eLife 7:e40018. DOI: https://doi.org/10.7554/eLife.40018,PMID: 30033910. Guasto JS, Johnson KA, Gollub JP. ... 2009. The Chlamydomonas Sourcebook. 2nd edition. London: Academic Press.Hinchliff CE, Smith SA, Allman JF, Burleigh JG, Chaudhary R, Coghill LM,

  5. 3 The Harmonic Oscillator I now want to use ...

    www.damtp.cam.ac.uk/user/dbs26/PQM/chap3.pdf
    18 Oct 2019: non-negative, because. n = nhn|ni = hn|N |ni = hn|A†A|ni = kA|nik2 0 (3.11). ... Taking the norm of both sides shows that. |cn|2 = kA†|nik2 = hn|AA†|ni = hn|N 1|ni = n 1.

  6. This isa spec ific indiv idual’s copy of the ...

    www.damtp.cam.ac.uk/user/sjc1/teaching/Waves/notes.pdf
    22 Aug 2019: c0= ka 1 ,. a ‘small’ sphere to be one such that a 2πc0ω. , ... i.e.ωa. c0= ka 1 ,. Mathematical Tripos: Part II Waves 16 S.J.Cowley@maths.cam.ac.uk, Lent 2019.

  7. 10. Scattering Theory The basic idea behind scattering theory ...

    www.damtp.cam.ac.uk/user/tong/aqm/aqmten.pdf
    19 Jul 2019: q. kA(eiqa/2 eiqa/2). Notice that only the combination (r t) appears.

  8. 4. Phonons Until now, we’ve discussed lattices in which ...

    www.damtp.cam.ac.uk/user/tong/aqm/aqmfour.pdf
    19 Jul 2019: 2=. mM. hm M. p(m M)2 4mM cos2(ka). i. The resulting dispersion relation is sketched in Figure 57 in the first Brillouin zone. ... This is because it is. valid only at long wavelengths, ka 1.

  9. 3. Electron Dynamics in Solids In the previous chapter ...

    www.damtp.cam.ac.uk/user/tong/aqm/aqmthree.pdf
    19 Jul 2019: structure. E = C cos(ka). Then the velocity in a constant electric field oscillates as. ... v(k) =Ca. sin(ka) = Ca. sineEa t. The Bloch frequency is! =

  10. 2. Band Structure In this chapter, we start our ...

    www.damtp.cam.ac.uk/user/tong/aqm/aqmtwo.pdf
    19 Jul 2019: value. E = E0 2t cos(ka) (2.5). The spectrum is shown in the figure for t > 0.

  11. 15632687789062 1..20

    www.damtp.cam.ac.uk/user/gold/pdfs/universal_swimming.pdf
    16 Jul 2019: eLife 7:e40018. DOI: https://doi.org/10.7554/eLife.40018,PMID: 30033910. Guasto JS, Johnson KA, Gollub JP. ... 2009. The Chlamydomonas Sourcebook. 2nd edition. London: Academic Press.Hinchliff CE, Smith SA, Allman JF, Burleigh JG, Chaudhary R, Coghill LM,

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