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  2. Publications | Astrophysics

    www.damtp.cam.ac.uk/research/astro/publications?page=24
    18 Jun 2024: KA Mizerski, K Bajer, HK Moffatt. – Journal of Fluid Mechanics.
  3. Publications | Soft Matter

    www.damtp.cam.ac.uk/research/softmatter/publications?page=16
    18 Jun 2024: E Sanz, KA White, PS Clegg, ME Cates. – Phys Rev Lett.
  4. topicsinqm

    www.damtp.cam.ac.uk/user/tong/aqm/topics6.pdf
    18 Sep 2022: q. kA(eiqa/2 eiqa/2). Notice that only the combination (r t) appears.
  5. D19a.dvi

    www.damtp.cam.ac.uk/user/examples/D19a.pdf
    15 Jan 2024: Show that the phase shifts δl obey. tanδl =jl(ka). nl(ka). 4. ... Show that the phase shifts obey. tanδl =q jl(ka)j. ′l(qa) k j.
  6. Publications | Maciej Dunajski | University of Cambridge

    www.damtp.cam.ac.uk/user/md327/publ.html
    20 May 2024: Dunajski, M. and Ka'zmierczak, M. (2007) Moduli spaces with external fields', hep-th/0610220.
  7. Einstein–Maxwell Gravitational Instantons Maciej Dunajski(joint work…

    www.damtp.cam.ac.uk/user/md327/Einstein_Maxwell_sydney.pdf
    29 Jul 2007: Ka = αAβ̂A′ α̂AβA′ is a Killing vector, and deduce the form of themetric.
  8. 13 Mar 2019: δ(r a). Show that the phase shifts are given by. tan δl = kλa2[jl(ka)]. ... 2. 1 kλa2jl(ka)nl(ka). [Hint: The δ-function leads to two continuity conditions at r = a.
  9. 3. Electron Dynamics in Solids In the previous chapter ...

    www.damtp.cam.ac.uk/user/tong/aqm/aqmthree.pdf
    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! =
  10. Geometric tuning of self-propulsion for Janus catalytic particles

    www.damtp.cam.ac.uk/user/lauga/papers/133.pdf
    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.
  11. Secure state-estimation for dynamical systemsunder active adversaries …

    www.damtp.cam.ac.uk/user/hf323/security_allerton2011.pdf
    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

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