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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!

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

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.

23 May 2024: 24. Residual DMD (ResDMD).

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.

20 May 2024: Slide 23: Example: Verified spectra and modes. Slide 24: Example: Verified dictionary.

26 Jun 2024: 255 –. Figure 24. A colour coded description of the possible ordering of neutrino masses. ... The two possibilities are shown in Figure 24. Given the pattern seen in all other.

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.

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.

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.