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  2. statphys

    www.damtp.cam.ac.uk/user/tong/statphys/two.pdf
    31 Dec 2018: Zvib =1. 2. Zddpe. Hvib =kBT! (2.20). The average vibrational energy of each molecule is now.
  3. Quantum Field Theory II University of Cambridge Part III ...

    www.damtp.cam.ac.uk/user/dbs26/AQFT/chap1.pdf
    19 Jan 2018: 2.2 Free field theory 14. 2.3 Perturbation theory 17. 2.3.1 Feynman diagrams 20. ... D eS[]/. (1.20). evaluates the map acting on |'0i 2 H and ending on |'1i 2 H.
  4. Topics in Convex Optimisation (Michaelmas 2018) Lecturer: Hamza Fawzi …

    www.damtp.cam.ac.uk/user/hf323/M18-OPT/lecture13.pdf
    13 Nov 2018: Q =. . q00,00 q00,10 q00,01 q00,20 q00,11 q00,02q10,10 q10,01 q10,20 q10,11 q10,02. ... q01,01 q01,20 q01,11 q01,02q20,20 q20,11 q20,02. q11,11 q11,02q02,02. . (2). 2.
  5. Preprint typeset in JHEP style - PAPER VERSION Easter ...

    www.damtp.cam.ac.uk/user/examples/B6La.pdf
    19 Sep 2018: 5. Functionals and the Euler-Lagrange equation 20. 5.1 Geodesics of the Euclidean plane 22. ... 20 –. for the integral (a real number) does depend on the function y.
  6. Metrisability of Painlevé equations

    www.damtp.cam.ac.uk/user/md327/cd18.pdf
    10 Mar 2018: In the recent work,20 some connections between the Painlevé property and Lie point sym-metries have been uncovered. ... Nonlinear Math. Phys. 20, 110 (2013).19 Koenigs, M. G., Sur les Géodesiques a Intégrales Quadratiques.
  7. Sound propagation in an irregular two-dimensional waveguideMark…

    www.damtp.cam.ac.uk/user/ms100/PAPERS/JASA97.pdf
    13 Dec 2018: 1997 Acoustical Society of America.@S0001-496697!03703-X#. PACS numbers: 43.20.Fn, 43.20.Mv, 43.30.Hw@ANN#. nsemismiceThthaceinionti-. ... An5an ,bn!, Cn5cn ,dn!, 20! wherean , bn , cn , dn are given by11!
  8. Research Article Journal of the Optical Society of America ...

    www.damtp.cam.ac.uk/user/ms100/PAPERS/rough-surface-reconstruction.pdf
    13 Dec 2018: 20). where Xl = 12 (xl1 xl). The last subintegral with singularitycan be approximated by. ... Then everything turns to be knownin Eq. (20) except the discrete ψ′(Xl).
  9. Statistical moments for rough surface scatter from two-way parabolic…

    www.damtp.cam.ac.uk/user/ms100/PAPERS/pebacksc-JModOpt.pdf
    13 Dec 2018: 21). Now from eq. (20). E(X,x) =〈h(X). α2π. d. dx. ... Soc. Lond. A 446 (1994) 1-20. (12) C. Qi, Z. Zhao, W.
  10. ✿ ✳ ✳ ✿ ✳ ✳✹✹ ✹✹ ✿ ✳ ...

    www.damtp.cam.ac.uk/user/mem/papers/LHCE/nothing.pdf
    7 Oct 2018: cresc. 1. 15. 20. 25. 30. ❲ ❲ ❲❲ ❲❲ ❲ ❲ ❲ ❲ ❲ ❲ ❲. ❲ ❲ ❲ ❲ ❲ ❲ ❲ ❲ ❲ ❲ ❲ ❲ ❲ ❲. ❲❲ ❲ ❲ ❲ ❲ ❲ ❲ ❲ ❲ ❲ ❲ ❲ ❲ ❲ ❲ ❲ ❲ ❲ ❲ ❲ ❲ ❲ ❲. ❲ ❲ ❲ ❲ ❲
  11. Time Irreversibility and Criticality in the Motility of a Flagellate…

    www.damtp.cam.ac.uk/user/gold/pdfs/gaitswitch.pdf
    3 Aug 2018: Thus, Ṡ quanti-fies the lack of detailed balance in the nonequilibrium steadystate, which, as reported elsewhere [20], depends on envi-ronmental conditions, emphasizing the need to account ... 19] J. Schnakenberg, Rev. Mod. Phys. 48, 571 (1976).[20] K.

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