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41 - 50 of 61 search results for katalk:za31 24 / / / / / |u:www.damtp.cam.ac.uk where 0 match all words and 61 match some words.

  1. Results that match 1 of 2 words

  2. munich_talk_mjc

    www.damtp.cam.ac.uk/user/mjc249/talks/rigged_DMD_munich.pdf
    10 Jun 2024: Slide 24: Spectral measures goes to diagonalisation. Slide 25: Spectral measures goes to dynamics.

  3. italy_mjc

    www.damtp.cam.ac.uk/user/mjc249/talks/Italy_mpEDMD.pdf
    6 Apr 2024: Slide 23: Convergence of measures. Slide 24: Further convergence. Slide 25: Lorenz system.

  4. cosmo

    www.damtp.cam.ac.uk/user/tong/cosmo/three.pdf
    26 Jun 2024: 1. ar v̇ = Ḣ. 1. arv̇. Take the gradient of (3.24) to get. ... 1.24). In such a situation, it would make little sense to talk about perturbations with.

  5. 7. Quantum Field Theory on the Line In this ...

    www.damtp.cam.ac.uk/user/tong/gaugetheory/72d.pdf
    26 Jun 2024: 4i. 1 log. i. 2UV. iv2. (7.24). where, to reach the second line, we’ve Taylor expanded in /2UV. , ... 2. This is the same kind of integral that we met in (7.24) when solving the 2d CPN1.

  6. 3. Introducing Riemannian Geometry We have yet to meet ...

    www.damtp.cam.ac.uk/user/tong/gr/three.pdf
    31 May 2024: Claim:. d? F =? J , rµF µ = J (3.24).

  7. 6. Black Holes Black holes are among the most ...

    www.damtp.cam.ac.uk/user/tong/gr/six.pdf
    31 May 2024: 6. Black Holes. Black holes are among the most enigmatic objects in the universe. They are described. by deceptively simple solutions to the Einstein equations, yet hold a host of insights. and surprises, from the meaning of causal structure, to

  8. Koopman_turing_talk_mjc

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

  9. 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.

  10. BMC_talk_mjc

    www.damtp.cam.ac.uk/user/mjc249/talks/rigged_DMD_manchester.pdf
    18 Jun 2024: 𝑒𝑗 𝑒𝑗1. 𝑈 =. Back to the shift! ෍. 24. 0 1. ... Slide 24: Back to the shift! Slide 25: Back to the shift!

  11. 2. Introducing Di↵erential Geometry Gravity is geometry. To fully ...

    www.damtp.cam.ac.uk/user/tong/gr/two.pdf
    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

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