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Effective approximation for the linear time-dependent Schrödinger…
www.damtp.cam.ac.uk/user/na/NA_papers/NA2012_05.pdf16 Jul 2012: 24 P. Bader, A. Iserles, K. Kropielnicka & P. Singh. of accuracy exhibited in Figs 4.3–4 is clearly in excess of O(ε7/2. ), -
ISlecture_notes_2012_part1.dvi
www.damtp.cam.ac.uk/user/md327/ISlecture_notes_2012.pdf10 May 2012: 24. 2.2 Inverse scattering transform for KdV. 252.2.1 Direct scattering. 272.2.2 Properties of the scattering data. ... dx. 24. Figure 2.1: Sine–Gordon Kink. Kink. x. Note that the Sine–Gordon equations didn’t enter the discussion at this stage. -
Manuscript submitted to Website: http://AIMsciences.orgAIMS’…
www.damtp.cam.ac.uk/user/na/NA_papers/NA2012_08.pdf5 Sep 2012: 7.1. A new scheme of Dirichlet series for particular systems of the form(24). ... Byletting z = P 1y, the system (24) is equivalent to a transformed dynamical system. -
Forces between single pairs of charged colloids in aqueous ...
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/ufk_papers/charged_membranes/dlvo-ot.pdf3 Oct 2012: Chem. Phys. 81, 6320 1984. 24 E. Allahyarov, H. Lowen, and S. -
The development of concentration gradients in a suspension of…
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/HillesdonPedleyKessler95.pdf2 Sep 2012: and, by equation (24) and the integral (21),. dO _f12. d z (0)= (27). ... terms in equation (23) and the oxygen consumption term in equation (24) are zero. -
The hydrodynamics of swimming microorganisms
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/LaugaPowers09.pdf27 Aug 2012: For example, it is nowpossible to measure the force required to hold a swimmingspermatozoon [24–26], alga [27] or bacterium [28] in an opticaltrap. -
Part II Applications of Quantum MechanicsLent 2012 Prof. R.R. ...
www.damtp.cam.ac.uk/user/rrh/notes/aqm_notes_180112.pdf8 Mar 2012: 23. 4.1.3 The optical theorem. 24. 4.1.4 Solving for the asymptotic scattered wave. ... 4 QUANTUM SCATTERING IN 3D 24. where δl is a function of k. -
Holographic Dual of the Lowest Landau Level David Tong ...
www.damtp.cam.ac.uk/user/tong/talks/hololll.pdf15 Oct 2012: Aspects of fermions in magnetic AdS geometries. have been previously discussed in [20, 21, 22, 23, 24]. -
Pattern formation in a suspension of swimming microorganisms:…
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/ChildressLevandowskySpiegel75.pdf2 Sep 2012: 2 3 ) pDV-D'@iF28@ = 0, (2.24). D(D = 0, x = - 1 , o. ( ... To see how these expansions proceed, we first note that (2.24) may be integrated, using (2.25), to dbtain 0 so CDdS(76Z2)/ -1 V d Z = 0. -
qjmam0117.tex
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/MagarGotoPedley03.pdf2 Sep 2012: NUTRIENT UPTAKE BY A SELF-PROPELLED STEADYSQUIRMER. by VANESA MAGAR†. (Department of Applied Mathematics and Theoretical Physics, University of Cambridge,Silver Street, Cambridge CB3 9EW). TOMONOBU GOTO. (Department of Mechanical Engineering,
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