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www.damtp.cam.ac.uk/user/mrep/webpubs.pdf11 Mar 2024: The kinematics of hexagonal magnetoconvection. Geo.Astro. Fluid Dyn., 24:109–136, 1983. 24. ... Phys. Fluids, 24,107103, 2012. 1975-1980 1981-1990 1991-2000 2001-2010 2011-2020 2021-2030. 184. -
Controlling Confined Collective Organization with Taxis
www.damtp.cam.ac.uk/user/lauga/papers/224.pdf21 Mar 2024: Pedley and J. Kessler, Annu. Rev. Fluid Mech. 24, 313(1992). [16] B. ... 24] A. Creppy, F. Plouraboué, O. Praud, X. Druart, S. Cazin, H.Yu, and P. -
Stochastic Voronoi Tessellations as Models forCellular Neighborhoods…
www.damtp.cam.ac.uk/user/gold/pdfs/Srinivasan_etal110324.pdf11 Mar 2024: 33, 958–972 (1962). [24] P. Rathie, On the volume distribution of the typi-cal Poisson–Delaunay cell, J. -
CV: Matthew J. ColbrookEMAIL: m.colbrook@damtp.cam.ac.ukWEBSITE:…
www.damtp.cam.ac.uk/user/mjc249/pdfs/CV_MColbrook2024.pdf11 May 2024: 24. M.J. Colbrook, B. Roman, A.C. Hansen, How to compute spectra with error control, Physical Review Letters,2019.Cover highlight for issue.Prizes: Grade 1 Smith–Knight/Rayleigh–Knight -
Opto-fluidically multiplexed assembly and micro-robotics
www.damtp.cam.ac.uk/user/lauga/papers/223.pdf28 Feb 2024: With rapid implementation and advanced control,it might be feasible to position one particle every fewmicrometers, which is the typical length scale over whichthe flow fields exhibit significant decay22,24. ... eLight 1, 7 (2021). 24. Liao, W. et al. -
Quantum Mechanics David Tong Department of Applied Mathematics and ...
www.damtp.cam.ac.uk/user/tong/qm/qm1.pdf20 Apr 2024: 2.1.2 The Infinite Potential Well 24. 2.1.3 The Gaussian Wavepacket 27. -
Koopman_turing_talk_mjc
www.damtp.cam.ac.uk/user/mjc249/talks/rigged_DMD_turing.pdf23 May 2024: 24. Residual DMD (ResDMD). -
Koop_italy_mjc
www.damtp.cam.ac.uk/user/mjc249/talks/Koopman_workshop_mjc.pdf20 May 2024: Slide 23: Example: Verified spectra and modes. Slide 24: Example: Verified dictionary. -
2 A Quantum Particle in One Dimension There is ...
www.damtp.cam.ac.uk/user/tong/qm/qm2.pdf20 Apr 2024: d2h. dy22ydh. dy+ (Ẽ 1)h = 0 (2.26). You can check that this is indeed satisfied by our earlier solution (2.24) with h = 1. ... We learn that the. Gaussian wavefunction (2.24) that we guessed earlier is actually the lowest energy. -
Preprint typeset in JHEP style - HYPER VERSION Michaelmas ...
www.damtp.cam.ac.uk/user/tong/qft/qft.pdf20 Mar 2024: where Λµν satisfies. Λµσ ηστ Λντ = η. µν (1.24). For example, a rotation by θ about the x3-axis, and a boost by v < 1 along the x1-axis. ... The condition (1.24) for Λ to be a Lorentz transformation. becomes. (
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