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4 Oct 2023: straightforward:. xinst() = a tanh!( 1). 2. (2.24). The profile of the instanton is shown in Figure 5. ... It follows. from the fact that, as seen in the explicit instanton profile (2.24), the instantons come.

28 Nov 2023: An incomplete list of examples includes most types of computational imaging[2, 14, 25], matrix completion [28], parametric PDEs/system identification [1], phase retrieval [30, 46, 86],quantized sampling [24] etc.

16 Sep 2023: P(x, t;x0, t0) =. Z 1. 1d3x,0P(x, t;x0, t0) P(x0, t0;x0, t0) (3.24). ... Kolmogorov equation (3.24). P(x, t;x0, t0) =. Z 1. 1d3x,0P(x, t;x0, t0) P(x0, t0;x0, t0).

11 Mar 2024: They solved their lubrication equations(24–32), again by an expansion in a small Deborah number We 1, going tothe first correction.

13 Sep 2023: defined as. 2xy = µ , x2 y2 = (2.24). The coordinates µ and are curvilinear and orthogonal (i.e. ... 24 –. Galilean group that we met in section 1.2.

8 Jun 2023: As explained in [23, 24], many variants of Koopman algorithms exist. ... 102. 103. 104. 14. 16. 18. 20. 22. 24. 26. 28.

1 Dec 2023: Nevertheless, in the dewatering of suspensions. 2469-990X/2022/7(5)/054303(24) 054303-1 2022 American Physical Society. ... More specifically, as a prescription for the stress in the solid phase,we employ a particular model formulated by Saramito [24]

2 Jul 2023: Slide 21: How? Slide 22: How? Slide 23: How? Slide 24: Adaptive computation of z superscript base , open paren cap A.

1 Dec 2023: dJ. dz= 1, that is J(z) = z. (24). In the asymptotic regime of high Rayleigh number, we expect that the heat producedis carried away by advection only, apart from the ... z⟩ =269. 1/2 and ⟨zθ⟩ = θ from (23) and (24).

22 Feb 2024: 1)f1(r, p. ′2) f1(r, p)f1(r, p2). ](2.24). This is the Boltzmann equation.