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  2. Koopman_turing_talk_mjc

    www.damtp.cam.ac.uk/user/mjc249/talks/rigged_DMD_turing.pdf
    23 May 2024: 24. Residual DMD (ResDMD).
  3. Koop_italy_mjc

    www.damtp.cam.ac.uk/user/mjc249/talks/Koopman_workshop_mjc.pdf
    20 May 2024: Slide 23: Example: Verified spectra and modes. Slide 24: Example: Verified dictionary.
  4. standardmodel

    www.damtp.cam.ac.uk/user/tong/sm/standardmodel6.pdf
    31 May 2024: 6.24). Of these, U(1)3 acts on V22, leaving the overall sum 1 2 3 4 unchanged.
  5. 31 May 2024: S T)µ1.µp1.r1.q1.s. = Sµ1.µp1.qT1.r. 1.s (2.24). Given an (r, s) tensor T , we can also construct a tensor of lower rank (r
  6. J. Fluid Mech. (2024), vol. 988, A11, doi:10.1017/jfm.2024.260 Fast…

    www.damtp.cam.ac.uk/user/hinch/publications/JFM988_A11.pdf
    31 May 2024: They solvedtheir lubrication equations (24)–(32), again by an expansion in a small Deborah numberWe 1, going to the first correction. ... p/. (1. c). p 1. De. H = 21/22. 23/24. Figure 1.
  7. standardmodel

    www.damtp.cam.ac.uk/user/tong/sm/standardmodel4.pdf
    31 May 2024: Tr T ART BR. =1. 2I(R)AB. (4.24). The Dynkin index is related to the quadratic Casimir C(R), which we previously defined.
  8. Preprint typeset in JHEP style - HYPER VERSION Michaelmas ...

    www.damtp.cam.ac.uk/user/tong/sft/sft.pdf
    12 Apr 2024: 1.3.1 The Landau-Ginzburg Free Energy 24. 1.3.2 The Saddle Point and Domain Walls 26.
  9. 31 May 2024: should identify. g00(x) (1. 2Φ(x). c2. )(1.24). where Φ(x) is the Newtonian gravitational field. ... 1.24) but with a linear gravitational potential Φ of the kind that we would invoke for.
  10. Preprint typeset in JHEP style - PAPER VERSION June ...

    www.damtp.cam.ac.uk/user/tong/tasi/tasi.pdf
    31 May 2024: 1.4.1 The Metric on the Higgs Branch 23. 1.4.2 Constructing the Solutions 24. ... in 5 1 dimensions is a sigma-model on a hyperKähler target space [24] which, for.
  11. 4. The Einstein Equations It is now time to ...

    www.damtp.cam.ac.uk/user/tong/gr/four.pdf
    31 May 2024: ṙ2 Ve(r) = E2 (4.24). but this time with the eective potential. ... This tells us that the particle follows a null geodesic. The equation (4.24) gets replaced.

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