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21 Oct 2020: Thus, with k = t ,. Euler: yn = (I kA)ny0, 1 z = e. ... z O(z 2);. TR: yn =[(. I 12 kA)1 (. I 12 kA)]n.

13 Mar 2019: δ(r a). Show that the phase shifts are given by. tan δl = kλa2[jl(ka)]. ... 2. 1 kλa2jl(ka)nl(ka). [Hint: The δ-function leads to two continuity conditions at r = a.

26 Jun 2024: H =1. 2a. Z /a. /a. dk. 22 sin(ka) c†. kck. – ... E(k) =1. asin(ka). This gives a dispersion relation of the kind we anticipated above: it has zeros at both.

8 Oct 2004: He found that, provided ka 1, where a is the core radius,σ2 =. ( κ2πh2. )2 [1 khK1(kh) 12(kh). 2ω(akδ)]. [1 khK1(kh) (kh)2K0(kh) ... Classical Crow instability. Crow used the cut-off method to determine the growth rate, σ , of the instability in

8 Jun 2009: These. parameters ka and kr are determined as the best fit parameters to the measurement (Fig. ... θmda = 107,θe = 90, θmdr = 77, ka = 9.0 109 and kr = 9.0 108 are used.

26 Oct 2020: Thus,. with k = t,. Euler: yn = (I kA)ny0, 1 z = e.

19 Oct 2013: Another importantwave activity measure is given by the pseudomomentum vector,. p = kA =h′ u′. ... Because of the ray-invariance of absolute frequency we have that |kA| = |kB | asympto-tically.

27 Feb 2018: PHYSICAL REVIEW E 97, 022411 (2018). Microbial mutualism at a distance: The role of geometry in diffusive exchanges. François J. Peaudecerf,1, Freddy Bunbury,2 Vaibhav Bhardwaj,2 Martin A. Bees,3 Alison G. Smith,2. Raymond E. Goldstein,1,† and

23 Sep 2015: along the anterior (kA = 1000 μm, hA0 = 0:8) and strongly along the posterior-lateral cortex (kP = 150 μm, hP0 = 0, see ‘Materials and methods’ MT nucleation. ... the inset of panel C (yellow circles). In all panels, parameter values for anterior

12 Jul 2024: Electron excitation of Be-like Fe XXIII for the n=2,3,4 configurations. MC Chidichimo, G Del Zanna, HE Mason, NR Badnell, JA Tully, KA Berrington. –