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  2. DAMTP 2010/NA04 Beyond symmetric Broyden for updating quadratic…

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2010_04.pdf
    13 Apr 2011: and y+. 4=. (20. ), (3.4). 8. with t = 4, θ = 0 and v = xk1 = xk = y1. , ... 5000 and n 20, but,for n = 10, the norms ‖Ek‖F become of the magnitude of computer roundingerrors in the difference 2Qk2F.
  3. Broken particle-hole symmetry in critical fluids Raymond E.…

    www.damtp.cam.ac.uk/user/gold/pdfs/broken_particle_hole.pdf
    10 Apr 2011: The effective Hamiltonian in Eq. (20) has odd (and momentum dependent) terms just like those in the simpli-fied field-theoretic model Eq. ... 20) onto the field-mixing operator. For this purpose, we note on general grounds and independent of the
  4. Emergence of Synchronized Beating during the Regrowth of Eukaryotic…

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/GoldsteinPolinTuval11.pdf
    30 Sep 2011: 2Department of Global Change Research, Mediterranean Institute for Advanced Studies (CSIC-UIB), E-07190 Esporles, Spain(Received 20 June 2011; published 30 September 2011). ... 30 SEPTEMBER 2011. 148103-4. 20] S. Takada and R. Kamiya, Cell Motil.
  5. Model for phase equilibria in micellar solutions of non ...

    www.damtp.cam.ac.uk/user/gold/pdfs/JChemPhys_84_3367.pdf
    10 Apr 2011: 00. 2Xt/J - t/JI(1 - t/J) - L (Bt/JnIBt/J)/nM = 0 (20) n=1. ... 3. (a) Micelle size distribution for; = 0.08, M = 20, E = 0.85, and q = 3.
  6. VOLUME 84, NUMBER 7 P H Y S I ...

    www.damtp.cam.ac.uk/user/gold/pdfs/twirl.pdf
    10 Apr 2011: Vt Czr. Vss 11. zrs 3 rss? fs. (4). The second term of (4) is nonzero [20] when the filamentis both out of elastic equilibrium f fi 0 and either ... Rubinow, J. Fluid Mech. 44, 705 (1976).[20] The writhe-tracking term is rs 3 rss?
  7. Generalized sampling and the stable and accuratereconstruction of…

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2011_12.pdf
    22 Nov 2011: f fn,m‖R (1 θ2. )‖f Qnf‖R c(2 θ)θ2|||f Qnf|||, (2.20). and thatκ(A). ... 12. The estimate (2.20) for ‖f fn,m‖ holds with the stronger assumption (A2′).
  8. Trapping and Wiggling: Elastohydrodynamics of Driven Microfilaments…

    www.damtp.cam.ac.uk/user/gold/pdfs/trapping.pdf
    10 Apr 2011: We note from the solution (Eq. 20) that each modegkdecays independently and exponentially with time. ... 0.485ỹ; yk2(0). 20.012ỹ, where we defineykn [ 0. 1 da y0kn, in analogy toEq.
  9. INSTITUTE OF PHYSICS PUBLISHING JOURNAL OF PHYSICS A: MATHEMATICAL ...

    www.damtp.cam.ac.uk/user/gold/pdfs/wigner_jphysa.pdf
    10 Apr 2011: k. )x̂nk(p̂mx̂k). (20). Here, we have used the notation x̂ = x and p̂ iη/x, together with the identity proven byMcCoy [23] (see also appendix B). ... Interscience)[19] Fröhlich H 1967 Physica 37 215–26[20] Fröhlich H 1973 Riv.
  10. 10 Oct 2011: q κ(yβ, yα). κ(yα, yα)= r, p. κ(yβ, yα). κ(yα, yα)= r (1-20). ... 20. By essentially analogous reasoning, it is also possible to exclude the following two sub-diagrams (double arrows have not been included here).
  11. lec_notes.dvi

    www.damtp.cam.ac.uk/user/rrh/notes/qphys.pdf
    22 Dec 2011: 196.3.1 The Black-Body Distribution. 20. 6.4 Atomic Transitions. 22. 7 Lasers 237.1 A model for the laser. ... The corollary is that if radiation is in contact. 6 QUANTUM STATISTICAL PHYSICS 20.

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