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11 Mar 2024: J. Baumberg, "Coupled counter-rotating polariton condensates in optically defined annular potentials", 111(24):8770-5 Proceedings of National Academy of Siences, USA (2014). ... 1-24, July 1997. Department of Applied Mathematics and Theoretical Physics,

3 Jul 2024: 2.3.1 The Gravitational Field 22. 2.3.2 Escape Velocity 24. 2.3.3 Inertial vs Gravitational Mass 25.

10 Jun 2024: Slide 24: Spectral measures goes to diagonalisation. Slide 25: Spectral measures goes to dynamics.

1 Dec 2023: in figures 11 and 12. Figure 11 shows profiles of samples with different ageing timesTage on inclines of 20; figure 12 shows profiles on slightly steeper inclines of 24.As a

20 Mar 2024: where Λµν satisfies. Λµσ ηστ Λντ = η. µν (1.24). For example, a rotation by θ about the x3-axis, and a boost by v < 1 along the x1-axis. ... The condition (1.24) for Λ to be a Lorentz transformation. becomes. (

16 Sep 2023: i(2.24). This is the Boltzmann equation. It’s not an easy equation to solve! ... 24 –. things change for quantum particles. We’ll keep the assumption of molecular chaos,.

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

19 Sep 2023: Too little ortoo much arousal results inpoorer performance. 24. • Inf.-dim. ... Slide 24: Example: Verified modes. Slide 25: Example: Verified modes. Slide 26: Example: Verified dictionary.

1 Dec 2023: 𝑤(𝜍,𝑌) = 𝑊 & 𝑤𝜂(𝜍,𝑌) = 0, (24). here 𝜂 = 𝑌 are the bordering yield surfaces where the plug havepeeds 𝑊. ... For a free shear layer with 𝛶𝑛1 = 𝜅 = 0, there is a self-similarolution to (23) and (24) of the form. =

13 Sep 2023: e2 2. )(t. time. Figure 24: The fixed space frame and the moving body frame. ... 2, 000 12 = 24, 000 years. The actual value of the precession is 25, 700 years.

1 Dec 2023: 1a), and a hose thermal conduct-ivity of 0.24 W m1 K1. ... The yellow shade marks the 24 h period selected to define h0 (36 60 h post-breakthrough).

3 Oct 2023: Hint: Consider. exp(inθ).]. 14. The position of a particle moving in simple harmonic motion in one dimension isx = 7 24 cos 3t 7 sin 3t. ... a) Show that the displacement from the centre of motion can be written as <(X)where X = (24 7i)e3it.

20 Feb 2024: H. Fawzi, O. Fawzi, S. Scalet, Certified algorithms for equilibrium states of local quantum Hamiltonians, QIP'24.

16 Sep 2023: Im(!) =! (!20! 2)2 2!2. (4.24). This is an odd function. ... oscillator, we can now use the explicit form (4.24) to derive.

26 Jun 2024: in (1.24) because E = (0,0,E) lies parallel to the side of the torus, not perpendicular. ... Instead, both (1.23) and (1.24) are best thought of as integrating the 2-form Fµν over.

12 Dec 2023: movement [24].

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.

26 Jun 2024: where. Kµ = µtr. A@A. 2i. 3AAA. (2.24). This means that, as in the Maxwell case, the theta term does not change the. ... derivative (2.24), the temporal component was K0 = 42W. For now, the key property of W(A) that we will need is.

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.

4 Oct 2023: Then, using our previous result (1.24), we have. Tr (1)F eH =X. ... 24 –. Note that we’re not assuming that all critical points of h correspond to true E = 0.