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26 Jan 2022: d loge RLdt. = αd loge M. dt,. whereα = 20.

4 Feb 2022: 0 10 20 30 40 5010. -15. 10-10. 10-5. 100. t. ... 40. -30. -20. -10. 10. 20. 30. 40. γ. δ@@R. Im(z).

9 Nov 2022: 093102-6. INSTABILITY OF AN ACTIVE FLUID JET. 20 40 60 80 100. ... The waving instability grows with time, with a larger amplitude when t =20.

11 Jun 2022: the stronger statement that (9) will hold forlarge enough d, using recent results from convex algebraicgeometry [18]–[20]. ... Instead we use a result from a more recent line of work[18]–[20].

13 Jun 2022: We will now describe. these, but won’t prove the equivalence with (4.20). ... quotient description of the vacuum moduli space (4.20). The general solution to the.

16 Jun 2022: in chapter 20 of Nair’s‘modern perspective on QFT’, or in ‘Symplectic geometry and geometricquantization’ by Blau. ... 0|[x̂, p̂]|0⟩ = i. (66). 20. States, observables and measurements. Unitarity, the Heisenberg picture and perturbation

7 Jul 2022: Examplesinclude the collapse of liquid or air bridges duringdewetting19,20 and air entrainment in dynamic wetting.21–23. ... 20 G. Reiter, Unstable thin polymer films: Rupture and dewet-ting processes, Langmuir, 1993, 9, 1344–1351.

3 Dec 2022: previous section. We computed the time-averaged radiated power in (6.20): it is given. ... q2/m! 2! 20 i! Here! 0 is the natural oscillation frequency of the atom while!

12 Mar 2022: 2. 0. – 2. – 4. – 6. – 8. 10 20 30 40 50 60 70 80 90 100. ... 0.2 3.7 0.7. 0.1 2.6 55.2. 0.5 20.7 0.7. 0.3 3.4 9.6 0.3.

16 Sep 2022: points,. Sij(r) = h(ui(x1) ui(x2))(uj(x1) uj(x2)i (6.20). Expanding out the four terms, the structure function can be trivially expressed in terms. ... obvious generalisation of (6.20),. Sijk(r) = h(ui(x1) ui(x2))(uj(x1) uj(x2)(uk(x1) uk(x2))i. – 235