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4 May 2023: 37.51 = 3751 102. Eg, for positive numbers, take A1  a  A2 and B  b < B+. ... A pA2 b. =b. A pA2 b. We can estimate this as bAC , which reduces the relative error.<latexit

24 Jul 2023: Hosseinidoust, B. Mostaghaci, O. Yasa, B.-W. Park, A. V. Singh, and M. ... Rasheed, and B. B. Jørgensen, Coral mu-. cus functions as an energy carrier and particle trap in the reef ecosystem, Nature (London) 428, 66(2004).

1 Dec 2023: B. B. B. B. y. (a) (b). (c) (d ). (e) ( f ). (g) (h). 1–1–2 0 2 –1–2–3–4–5–6 0. FIGURE 4. (Colour online) Flow around ... 1.0. 1.5. 2.0. 2.5. 51015202530. 10121416. 2468. Bxx. B B. y.

7 Dec 2023: 2ffiffiffiffiffiffibBp. =ar and g = (b/B)1/2 = ((B 1)/2B)1/2 Z 1. ... 7A and B) than itdoes for rod-like swimmers (Fig. 7C and D).

26 Jan 2023: In matrix notation, (1.5) then becomes. 1! B! B 1! J =. e2n. mE. We can invert this matrix to get an equation of the form. ... 1! B! B 1! (1.8). The o-diagonal components of the resistivity tensor, xy =! B/DC, have a couple. of rather nice properties.

13 Sep 2023: y = b. eB+ R cos (!(t t0)) (4.32). with a, b, R and t0 integration constants. ... terms of the gauge potential A. Since we define B = r A, we immediately have one.

26 Jul 2023: A and. B are both self-adjoint and that. Bis positive and invertible. ... We take the completion of this space,. HB1. D(B) is dense in.

14 Feb 2023: 2ffiffiffiffiffiffibBp. =ar and g = (b/B)1/2 = ((B 1)/2B)1/2 Z 1. ... 7A and B) than itdoes for rod-like swimmers (Fig. 7C and D).

18 Dec 2023: k1 andthat for some r (α1, 2k1) we have B(b, U, r). ... Moreover, Γ2 either fails on the whole of B(b, U, α1) or on another open set θ B(b, U, r).

16 Sep 2023: The Liouville equation is often written using the Poisson bracket,. {A, B} @A. ... in this picture. First, the impact parameter, b, is the distance from the asymptotic.