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16.4. PROBLEM SET IV 216 16.4 Problem Set IV ...
www.tcm.phy.cam.ac.uk/~bds10/aqp/ps4.pdf22 Nov 2009: and verify that the scattering is isotropic when the energy of the incidentparticle or the size of the scatterer is sufficiently low, so that Ka 1.Obtain an expression for the -
Publications 1980 - 1989
www.tcm.phy.cam.ac.uk/~mw141/1980.html13 Dec 2009: Phys. A18 3007-3026 (1985) (23) Frequency Dependence of NMR Spin-Lattice Relaxation in Bilayer Membranes JA Marqusee, M Warner and KA Dill, J. -
Daniel Rowlands
www.tcm.phy.cam.ac.uk/profiles/dar55/27 Feb 2018: Predicting Sizes of Hexagonal and Gyroid Metal Nanostructures from Liquid Crystal Templating KA Asghar, DA Rowlands, JM Elliott, and AM Squires ACS Nano 9(11) 10970-10978 2015. -
Alumni of TCM Group
www.tcm.phy.cam.ac.uk/about/alumni/1 Apr 2024: KA Kikoin (visitor 1994-95). RJ Kingdon (gs. 1986-87). DR Kingham (gs. -
Group Publicatons
www.tcm.phy.cam.ac.uk/publications/Pubs2014.htmlHybrid MPI-OpenMP Parallelism in the ONETEP Linear-Scaling Electronic Structure Code: Application to the Delamination of Cellulose Nanofibrils KA Wilkinson, NDM Hine and C-K Skylaris, J. ... KA See et al., J. -
lectures
www.tcm.phy.cam.ac.uk/~bds10/aqp/lec16-17.pdf17 Nov 2009: Substituted into the equations of motion, we obtain. (mω2 2ks ) = 2ks cos(ka). ... ksm| sin(ka/2)|. Classical chain: normal modes. ωk = 2. ksm| sin(ka/2)|. -
Group Publicatons
www.tcm.phy.cam.ac.uk/publications/Pubs2015.htmlKA Asghar, DA Rowlands, JM Elliott and AM Squires, ACS Nano 9 10970 - 10978 (2015). -
lectures
www.tcm.phy.cam.ac.uk/~bds10/aqp/lec2.pdf12 Oct 2009: κa =. {ka tan(ka) evenka cot(ka) odd. κa =. (2ma2V0! 2 (ka)2. ... leads to the condition,. k [An1 cos(ka) Bn1 sin(ka) An] =2maV0! -
NATURAL SCIENCES TRIPOS Part II Wednesday 13 January 2016 ...
www.tcm.phy.cam.ac.uk/~cc726/TP1/ExamFiles/exam16sol.pdf20 Jan 2016: 2mṙθ̇ mrθ̈ = ka sin(θ θB). d. dt. L. ṙ=L. ... r= mr̈ = mrθ̇2 kr ka cos(θ θB). d. dt. L. -
phmain
www.tcm.phy.cam.ac.uk/~bds10/phase/topol.pdf4 Apr 2010: The first indication of unusual behaviour in the two-dimensional XY -model (n = 2)appeared in an analysis of the high temperature series expansion by Stanley and Ka-plan (1971).
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