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3 Apr 2018: Magnus–Lanczos methods with simplified. commutators for the Schrödinger equation with a. time-dependent potential. Arieh Iserles, Karolina Kropielnicka† & Pranav Singh‡. April 4, 2018. AMS Mathematics Subject Classification: Primary 65M70,

20 Jan 2017: 2012 Wetting of flexible fibre arrays. Nature 482,510–513. (doi:10.1038/nature10779). 9. Wu X-F, Bedarkar A, Vaynberg KA.

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.

3 Oct 2017: Commutator-free Magnus–Lanczos methods for the. linear Schrödinger equation. Arieh Iserles, Karolina Kropielnicka† & Pranav Singh‡. October 3, 2017. AMS Mathematics Subject Classification: Primary 65M70, Secondary 35Q41,65L05, 65F60. Keywords

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,.

2 Sep 2012: gðrÞ azimuthal variation of the y-directed componentof the cytosolic velocity. Ka, Kb constants which appear in solving the parallelplate problem of Section 5.

25 Feb 2016: FL48CH05-Lauga ARI 24 November 2015 12:50. Bacterial HydrodynamicsEric LaugaDepartment of Applied Mathematics and Theoretical Physics, Center for MathematicalSciences, University of Cambridge, Cambridge CB3 0WA, United Kingdom;email:

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

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

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?

2 Sep 2012: Phys Rev Lett103:1981103. 15. Guasto JS, Johnson KA, Gollub JP (2010) Oscillatory flows induced by microorganismsswimming in two dimensions.

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

26 Jun 2024: automatically patched at x = a as well. We have. (x) cts at x = a ) B cos ka = Aea. ... plot the graph = k tan ka in blue, and then superpose this with the circle.

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

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

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

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,.

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.

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.

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

10 Apr 2011: 3). vs T = - l/Ka• Recall that this expression refers to the formulation in Eq. ... I(K1,K2 ,Ka) =! Ko+ In Tria,) exp[L: Keff(l- Oa,a /)] , (lJ) (16).

1 Sep 2011: i j is js s, |i| :=. s. is. The following lemmas will be used frequently (see [Ka], pp.

4 Jan 2024: Ex = ωA sin(nπy. a. ). sin(kz ωt). and. By = kA sin(nπy.

7 Jan 2013: Phys Rev Lett 105(16):168101. 17. Guasto JS, Johnson KA, Gollub JP (2010) Oscillatory flows induced by microorganismsswimming in two dimensions.

31 May 2023: Preprint typeset in JHEP style - HYPER VERSION Lent Term, 2017. Applications of Quantum MechanicsUniversity of Cambridge Part II Mathematical Tripos. David Tong. Department of Applied Mathematics and Theoretical Physics,. Centre for Mathematical

28 Oct 2006: This. isa. super. vis. or’. sco. py. ofth. enote. s.It. isnot. tobe. dis. trib. ute. dto. studen. ts. Natural Sciences Tripos: IB Mathematical Methods I. Contents. 0 Introduction i. 0.1 Schedule. i. 0.2 Books. ii. 0.3 Lectures. ii. 0.4 Printed

23 Sep 2015: along the anterior (kA = 1000 μm, hA0 = 0:8) and strongly along the posterior-lateral cortex (kP = 150 μm, hP0 = 0, see ‘Materials and methods’ MT nucleation. ... the inset of panel C (yellow circles). In all panels, parameter values for anterior

28 Nov 2013: J. Fluid Mech. (2013), vol. 737, pp. 205–231. c Cambridge University Press 2013 205doi:10.1017/jfm.2013.559. Stability of columnar convection in a porousmedium. Duncan R. Hewitt1,†, Jerome A. Neufeld1,2,3 and John R. Lister1. 1Institute of

7 Oct 2014: Anti-Self-Duality and Solitons. Prim PlansangkateTrinity College. University of Cambridge. Department of Applied Mathematics and Theoretical Physics. Faculty of Mathematics. Supervisor: Dr Maciej Dunajski. This dissertation is submitted for the

1 Dec 2023: T R A N S P O R T P H E N O M E N A A N D F L U I D M E C H A N I C S. On two-phase modeling of dewatering pulp suspensions. Daniel T. Paterson1 | Tom S. Eaves2 | Duncan R. Hewitt3 | Neil J. Balmforth4 |. D. Mark Martinez1. 1Department of Chemical

19 Oct 2013: Another importantwave activity measure is given by the pseudomomentum vector,. p = kA =h′ u′. ... Because of the ray-invariance of absolute frequency we have that |kA| = |kB | asympto-tically.

23 Oct 2023: Indeed, withk = t, we have:. Euler: un1 = (I kA)un, ez = 1 z O(z2);Implicit Euler: un1 = (I kA)1un, ez = (1 z)1 O(z2);.

6 Jul 2024: KA Mizerski, HK Moffatt. – Geophysical and Astrophysical Fluid Dynamics. (2018).

6 Jul 2024: R Hložek, EEO Ishida, J Guillochon, SW Jha, DO Jones, KS Mandel, D Muthukrishna, A O’grady, CM Peters, JR Pierel, KA Ponder, A Prša, S Rodney, VA Villar. –

2 Jul 2024: Preprint typeset in JHEP style - HYPER VERSION Lent Term, 2017. Topics in Quantum MechanicsUniversity of Cambridge Part II Mathematical Tripos. David Tong. Department of Applied Mathematics and Theoretical Physics,. Centre for Mathematical Sciences,.

10 Apr 2011: RAPID COMMUNICATIONS. PHYSICAL REVIEW E AUGUST 1997VOLUME 56, NUMBER 2. Elastohydrodynamic study of actin filaments using fluorescence microscopy. D. Riveline,1 C. H. Wiggins,2 R. E. Goldstein,3 and A. Ott1,1Laboratoire PhysicoChimie Curie,†

6 Oct 2014: Anti–self–dual fields. and manifolds. Moritz F. Högner. Trinity College. Dissertation submitted for the Degree of Doctor of Philosophy. October 2012. Abstract. Anti–self–dual fields and manifoldsMoritz F. Högner. In this thesis we study

5 Aug 2011: Although the strong correlationsuggests an almost constant and linear relationship, it actually appears as ifthe earliest part of the record (before about 650 ka) had lower mixing ratios(both absolutely and ... a) The last interglacial and methane. The

23 Apr 2021: q. kA(eiqa/2 eiqa/2). Notice that only the combination (r t) appears.

20 Sep 2011: ω 6= 0 so ω defines a Killing vector Ka.Killing identity Ka RabKb = 0, where Rab = gab/4. ... M|K|2gd4x = 1. 4. M|K|2gd4x. Therefore Ka = 0 and our assumption was wrong.

7 Apr 2021: 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! =

4 Oct 2013: if ψ = 0at r = a then Rnk(a) = Jn(ka) = 0 so for each n, ka = kni with i = 1, 2,.

10 May 2012: INTEGRABLE SYSTEMS. Maciej Dunajski. Department of Applied Mathematics and Theoretical Physics. University of Cambridge. Wilberforce Road, Cambridge CB3 0WA, UK. May 10, 2012. Contents. 1 Integrability in classical mechanics 41.1 Hamiltonian

6 Jul 2020: Cobalt yielded an intrinsic rema-nent magnetization of $ 500 kA/m. Other magnetic materials, such asparamagnetic iron oxide, could be utilized with a stronger magneticfield.

18 May 2022: Elastohydrodynamic Synchronization of Rotating Bacterial Flagella. Maria Tătulea-Codrean 1,2 and Eric Lauga 1,1Department of Applied Mathematics and Theoretical Physics, University of Cambridge,. Cambridge CB3 0WA, United Kingdom2Collège de France

30 Nov 2015: Mathematical Methods. University of Cambridge Part IB Mathematical Tripos. David Skinner. Department of Applied Mathematics and Theoretical Physics,. Centre for Mathematical Sciences,. Wilberforce Road,. Cambridge CB3 0WA. United Kingdom. d.b.skinner

26 Jun 2024: 2. Yang-Mills Theory. Pure electromagnetism is a free theory of a massless spin 1 field. We can ask: is it. possible to construct an interacting theory of spin 1 fields? The answer is yes, and the. resulting theory is known as Yang-Mills. The