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29 Dec 2023: Preprint typeset in JHEP style - HYPER VERSION. Statistical PhysicsUniversity of Cambridge Part II Mathematical Tripos. David Tong. Department of Applied Mathematics and Theoretical Physics,. Centre for Mathematical Sciences,. Wilberforce Road,.

27 Nov 2007: 0 ikeika ikeika k̃ek̃a.  = 0which yields. tan ka =2kk̃.

18 Nov 2002: "#$% &'(%!) ,# #-'(. / 102 &-! &3-! 45 6507(8% ":9 1 &;< =. >@?BA?DCFEG?IHJLKNMPOQCFRDSTMUV?DOWAYX1MZ[A R]U_UCFEaMb/c?dAYefMX?dAYEFgPhi?]Z_b/jkefMR]OlMPAYEFg?]C:m&eonphQEagh. q"Z_EsroMOQhlEtAunR]v? ]Xw_OYEabfxyM]z[{2EFCtw|MPOl}RDOYgMkRo?]bzLv?

10 Apr 2011: PACS: 87.17.d; 87.16.Ka; 05.45.a; 46.70.De. Keywords: Supercoil; Growth; Elastic filaments; Filamentous bacteria.

24 Apr 2014: and is characterized by four non-dimensional numbers:. Pe= kBTAλ2a. ηf D2, Da= Ka.

25 Sep 2015: FL47CH15-Goldstein ARI 1 December 2014 20:34. Green Algae as ModelOrganisms for BiologicalFluid DynamicsRaymond E. GoldsteinDepartment of Applied Mathematics and Theoretical Physics, Centre for MathematicalSciences, University of Cambridge,

10 Nov 2017: rspa.royalsocietypublishing.org. ReviewCite this article: Atiyah M, Dunajski M,Mason LJ. 2017 Twistor theory at fifty: fromcontour integrals to twistor strings. Proc.R.Soc.A 473: 20170530.http://dx.doi.org/10.1098/rspa.2017.0530. Received: 1 August

14 Feb 2005: Part II Statistical Mechanics, Lent 2005. Prof. R.R. Horgan. February 14, 2005. 1 Statistical Mechanics. 1.1 Introduction. The classical and quantum dynamics of simple systems with few degrees of freedomis well understood in that we know the

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! =

8 Nov 2017: a r t i c l e’s s u r f a c e τ τ ζ θ ζ ξ ζ = C kA D/ ( ) ( , ) (1 ) /0.

2 Sep 2012: 38. Guasto JS, Johnson KA, Gollub JP (2010) Oscillatory flows induced by microorganismsswimming in two dimensions.

10 Apr 2011: 0.6. xc. 0.5 ---- --------Xc«Mn)a CXl)---------. 0.4. 0.4 0.5 0.6. ka T lu.

27 Jul 2007: K bb Ka = 12ηKa. Thus K is automatically geodesic, and if it is pure then its trajectories are parameterizedby an affine parameter.

6 Oct 2016: Hencethere exists xa 6= x(0), and e(0)a ,. ,e(T1)a with supp(e(t)a ) Ka that generate the same sequence y(0),. ... y(T1) of ob-served values, with in addition, |Ka| |K| q. We thereforehave two different initial conditions x(0) 6= xa and twodifferent

17 Apr 2021: Preprint typeset in JHEP style - HYPER VERSION. Statistical PhysicsUniversity of Cambridge Part II Mathematical Tripos. David Tong. Department of Applied Mathematics and Theoretical Physics,. Centre for Mathematical Sciences,. Wilberforce Road,.

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,

3 Apr 2018: Vortices, Painlevé integrability andprojective geometry. Felipe ContattoQueens’ College. This dissertation is submitted for the degree of Doctor of Philosophy. Department of Applied Mathematics and Theoretical Physics. University of Cambridge.

25 Aug 2022: Preprint typeset in JHEP style - HYPER VERSION. F́ısica Estad́ıstica. David Tong. Department of Applied Mathematics and Theoretical Physics,. Centre for Mathematical Sciences. Wilberforce Road,. Cambridge, CB3 OBA, UK.

12 Aug 2016: Representing the resonance between the modes @n,o,ka and by the label (n, k,, k,,), the solid circles represent (n, 1,l) resonances; the solid squares (n, 2,2) resonances;

3 Oct 2008: Natural Sciences Tripos, Part IB. Michaelmas Term 2008. Mathematical Methods I. Dr Gordon Ogilvie. Schedule. Vector calculus. Suffix notation. Contractions using δij and ǫijk. Re-minder of vector products, grad, div, curl, 2 and their