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4 Jul 2024: Alex Chamolly ('16-'20) - now postdoc, ENS Paris and Institut Pasteur [Favourite movie: The Silence of the Lambs]. ... Weida Liao ('20) - from Trinity College, Cambridge [Favourite movie: Singin' in the Rain].

3 Jul 2024: Lecture notes. Woods Hole Oceanographic Institution GFD summer school: Shear Turbulence: Onset and Structure' 20 June - 26 August 2011, Woods Hole, Massachusetts. (

3 Jul 2024: 20. , 2060 (2024). [DOI]. Partial and complete wetting of droplets of active Brownian particles, arXiv:2310.07531. ... 20] R. L. Jack and P. Sollich, J. Stat. Mech. (2009), P11011.

29 Jun 2024: P. H. Htet and E. Lauga, J. Roy. Soc. Interface, 20, 20230428, 2023. ... W. M. Bush, A. E. Hosoi and E. Lauga, Phys. Fluids, 20, 082106, 2008.

4 Jul 2024: Goldstein. Physical Review Letters 64, 1043 (1990) [pdf]. 1989. 20. Parity-Breaking Transitions of Modulated Patterns in Hydrodynamic Systems.

3 Jul 2024: attractive or repulsive). – 63 –. bb. Figure 20:. Firstly, by energy conservation, the speed of the particle at the end of its trajectory. ... negligible. But, from (4.20), we see that, regardless of the initial velocity v, if you fire.

3 Jul 2024: 2.2.1 Central Forces 20. 2.2.2 Angular Momentum 21. 2.3 Gravity 22.

2 Jul 2024: 1.2.2 An Example: Spinless Particles 18. 1.2.3 Another Example: Spin 20. ... The. dual state h|A is defined by. (h|A)| i = h|(A| i) (1.20).

2 Jul 2024: We define the Rabi frequency as. = eE0 h 1|x| 2i (4.20). ... However, the Rabi frequency is proportional to the. amplitude of the electric field (4.20).

3 Jul 2024: 2.2.1 Central Forces 20. 2.2.2 Angular Momentum 21. 2.3 Gravity 22. ... 22 x. 23, from which we can. – 20 –. compute r/xi = xi/r for i = 1, 2, 3.

3 Jul 2024: 2.2.1 Central Forces 20. 2.2.2 Angular Momentum 21. 2.3 Gravity 22. ... 23, from which we can. – 20 –. compute @r/@xi = xi/r for i = 1, 2, 3.

2 Jul 2024: x0 = E/C. The asymptotic behaviour (2.19) and (2.20) is exactly what we need to. ... totic form of the Airy function (2.20) is given by. Ai(x).

2 Jul 2024: B =2µ03. mN3(0). µ04r3. (3(mN r̂)r̂ mN) (3.20). The second term is the long-distance magnetic field and was derived in Section 3 of. ... Hamiltonian. H = m B = emS B. For the s-wave, the contribution from the second term in (3.20) vanishes and we only

3 Jul 2024: 7. Special Relativity. Although Newtonian mechanics gives an excellent description of Nature, it is not uni-. versally valid. When we reach extreme conditions — the very small, the very heavy or. the very fast — the Newtonian Universe that

2 Jul 2024: equation. e2ik = 1 2ik. U0. (6.20). – 204 –. To understand the physics behind this, let’s first look at the situation where U0! ... We can expand (6.20) in 1/U0. (This too is left. as a problem on the exercise sheet.) We find.

2 Jul 2024: 2, 1)1/2 (5.20). where, again, the labelling is premature and should be taken with a grain of salt before. ... components of these doublets. We write. QL =. uL. dL! and LL =. L. eL! (5.77). (We already introduced these names in (5.18) and (5.20) although,

2 Jul 2024: It is given by. =eH. Z(5.20). where H is the Hamiltonian.

2 Jul 2024: 1.2.2 An Example: Spinless Particles 18. 1.2.3 Another Example: Spin 20. ... The. dual state ⟨ϕ|A is defined by. (⟨ϕ|A)|ψ⟩ = ⟨ϕ|(A|ψ⟩) (1.20).