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29 Apr 2024: Research. I'm Principal Investigator on our STFC Consolidated HEP theory grant: £2.3m ST/T000694/1 (1/10/20-30/9/24) and £2.2m ST/X000664/1 ... 20 Oct 2022: RD/RD interview in CERN Courier.

13 Jun 2024: Speaking (online) at XAI: Explaining what goes on inside DNN/AI (Oct 20, 2020). ... Speaking at Imperial College/University College London, Numerical Analysis Seminar (Feb. 20 2019).

26 Jun 2024: commutation relations (3.17) tell us that. [x̂, p̂] = i (3.20). ... Because. it follows purely from (3.20), any operators that obey the same commutation relation.

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. (

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].

8 Jun 2024: 01/01/17-. 31/12/20. , also. 01/01/07-. 31/12/14). ;. the Nominating Committee for External Members of the Council. ... 01/10/22-. 31/12/23. and. 01/01/16-. 31/12/17. , co-opted. 01/01/18-. 31/12/20. and. 01/01/08-.

18 Jun 2024: FoCM 2023. (Sorbonne University, Paris. 20 June 2023. Semi-Plenary Speaker (10th Popov Prize Lecture). ... Third Symposium on Machine Learning and Dynamical Systems. (Fields Institute. 20 Sep 2022.

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.

20 May 2024: 2023) Wormhole Model for Neon-20' arXiv:2303.15567. ... Quantum Grav. 20, 3427-3440. Dunajski, M. and Mason, L.J. (2003) Twistor theory of hyper-K{"a}hler metrics with hidden symmetries', J.

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.

22 Apr 2024: Nonlin. Processes Geophys., 20, 239-248. Haynes, P.H., 2013: Transport in geophysical fluids -- overview. ... Phys. Fluids, 19, 067101. (20 pages). Tzella, A., and Haynes, P.H., 2007: Small-scale spatial structure in plankton distributions.

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).

11 May 2024: 11:00-11:20 : Diana HalikiasElliptic PDE Learning Is Provably Data-Efficient. • 15:45-16:05 : Samuel Otto Operator learning without the adjoint. •

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).

18 Jun 2024: PDF. 163. Moffatt, H. K. 2007c Professor D. Howell Peregrine - 30 December 1938 - 20 March 2007.Obituary. ... 442, pp. 29–35. Springer. Symposium in Honour ofProfessor Jean-Pierre Guiraud, Université Pierre et Marie Curie, Paris, France, 20–22

26 Jun 2024: wavefunction as. (r) = rR(r) (4.20). Then, written in terms of the new function (r), the Schrödinger equation takes the. ... additional = 0 node. In Figure 20 we’ve fixed the energy level to n = 4 and plotted.

26 Jun 2024: in Figure 20. In the rest of this section, we will describe the basics of neutrino masses. ... As we saw in. Section 5, we label the three generations of leptons as (5.20),.

23 May 2024: 15. 20. 16. 20. 17. 20. 18. 20. 19. 20. 20. ... 17. 20. 18. 20. 19. 20. 20. 20. 21. New Papers on“Koopman Operators”.

26 Jun 2024: story for leptons? We decompose the left-handed leptons as (5.20). LiL=. ( ... i. L. (6.20). Each of these currents is diagonal in flavour, but this is before we do the rotation (6.9).

26 Jun 2024: 2.1 The Free Particle 20. 2.1.1 A Particle on a Circle 22.

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

26 Jun 2024: re-purpose it to describe atomic reactions like (2.20) (and, later, nuclear reactions). ... will understand recombination and the atomic reaction (2.20). We consider non-relativistic particles, with energy.

26 Jun 2024: 2.1 The Free Particle 20. 2.1.1 A Particle on a Circle 22. ... 20 –. If we do interpret (2.6) as the energy of the particle, we should probably compare it.

26 Jun 2024: action from (8.19). Se =. Zd3x. g2. 82(@µ). 2 KeSmono cos(2) (8.20). ... our eective action (8.20). This means that the vacuum does not support a constant,.

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.

18 Jun 2024: This allows us to compute the spectral measure associated with the dynamics of a protein molecule with a 20,046-dimensional state space and compute nonlinear Koopman modes with error bounds ... An IMA Leslie Fox Prize 2023. 20. M. Colbrook, L. Ayton, "A

12 Apr 2024: 1.2.4 A First Look at Universality 20. 1.3 Landau-Ginzburg Theory 22. ... χ 1|T Tc|. (1.20). We’ll see the relevance of this shortly.

26 Jun 2024:  2 Z+ (2.20). This is interesting. We have an example where a parameter in an action can only. ... freedom w() and the Lagrange multiplier (). First, we ask: how can we see the quantisation condition of  (2.20) in the path.

11 Jun 2024: Such methods offer certain advantages (forexample in high dimensional settings [20]), but are typically outperformed by traditional numericalmethods in accuracy in most settings [17]. ... 20] J. Han, A. Jentzen, and W. E. Solving high-dimensional partial

26 Jun 2024: conditions, Sθ can only take values of the form. Sθ = θN with N Z (1.20). ... 22cNe2. Sθ = θN with N = nn′ Z. which is our promised result (1.20).

26 Jun 2024: The. infinitesimal action of the vector rotation! ei is. = i , ̄ = i (3.20). ... tions dier. For the vector transformation (3.20), we have = i and ̄ = i ̄.This extra minus sign means that the Jacobian factors for and ̄ have the form.

31 May 2024: X0 = R sinh(/R) and Xi = R cosh(/R)yi (4.20). where the yi, with i = 1, 2, 3, 4, obeyP.

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

27 Apr 2024: 2.2.3 General Charge Distributions 20. 2.2.4 Field Lines 23. 2.2.5 Electrostatic Equilibrium 24. ... G(r; r′) = 14π. 1. |r r′|(2.20). – 20 –. We can now apply our usual Green’s function methods to the general Poisson equation.

6 Apr 2024: 15. 20. 16. 20. 17. 20. 18. 20. 19. 20. 20. ... 20. 21. New Papers on“Koopman Operators”. number of papers. doubles every 5 yrs.

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.

10 Jun 2024: 71, 481–495. 20. Hinch, E.J. 1975 Applications of the Langevin equation to fluid suspensionsJ. ... Fluids 20, 023302(9 pages). 119. Chiu-Webster, S., Hinch, E.J. & Lister, J.R.

12 Apr 2024: 2(ϕ)2 λ0 ζβ. 20/4π cos(β0ϕ. ). Hence show that the cos(βϕ) potential is relevant when β20 < 8π and irrelevant when.

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).

12 Jun 2024: solve this in conjunction with (4.20) but here it will turn out, somewhat fortuitously,. ... that if we just find the obvious solution to (4.20) then it solves rB = 0 automatically.

26 Jun 2024: 20 –. If we do interpret (2.6) as the energy of the particle, we should probably compare it. ... tem in Nature are described by the Hamiltonian (2.20). (There are exceptions.

1 May 2024: s2αs‖uχN‖r2α‖‖u(M)N χN‖s2α+ Er,s(M )‖V‖r2αr‖V‖s2αs‖uχN‖s2α‖‖u(M)N χN‖r2α. (20). ... 20) any term of the form ‖u χN‖t has t 0 (by virtue ofr,s 1 = 2α).

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,

31 May 2024: about an interesting person and having to spend the first 20 pages wading through. ... so, from (2.20),. the pull-back of a basis vector dxµ is.

26 Jun 2024: compute correlation functoins. hJ1. Jpic N1p/2 (6.20). The first factor of N comes from the planar diagrams with a quark loop running.

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.

26 Jun 2024: the emitted light,. 0 =a(t0). a(t1)1 =. 1. a(t1)(1.20). This is intuitive: the light is stretched by the expansion of space as it travels through. ... long journey. If they are emitted with frequency 1 then, from (1.20), they arrive with.

26 Jun 2024: This is achieved by the so-called hedgehog ansatz,. USkyrme(x) = exp (if(r) x̂) = cos f(r) i x̂ sin f(r) (5.20). ... a spatial and flavour rotation. The subgroup of (5.21) which acts non-trivially on the Skyrmion solution (5.20).

31 May 2024: which it couples to the new term Aµ(x). It’s simple to check that the action (1.20). ... 1.20) is determined by the Maxwell equation. We will describe the Einstein equations.