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15 Jan 2024: Show that the phase shifts δl obey. tanδl =jl(ka). nl(ka). 4. ... Show that the phase shifts obey. tanδl =q jl(ka)j. ′l(qa) k j.

6 Feb 2019: 2αβ. f. Qαg. Qβ. 1. 2ij. f. qig. qj,. Isometries are generated by Killing potentials KA(Q+,q+,u) that obey the. ... conservation law” KA {KA,L(4)} = 0. L(4) =P(4)(Q+). (qu)2. P(4)(Q+) = 112.

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.

6 Oct 2016: Hencethere exists xa 6= x(0), and e(0)a ,. ,e(T1)a with supp(e(t)a ) Ka that generate the same sequence y(0),. ... y(T1) of ob-served values, with in addition, |Ka| |K| q. We thereforehave two different initial conditions x(0) 6= xa and twodifferent

19 Jul 2019: structure. E = C cos(ka). Then the velocity in a constant electric field oscillates as. ... v(k) =Ca. sin(ka) = Ca. sineEa t. The Bloch frequency is! =

20 Oct 2019: eLife 7:e40018. DOI: https://doi.org/10.7554/eLife.40018,PMID: 30033910. Guasto JS, Johnson KA, Gollub JP. ... 2009. The Chlamydomonas Sourcebook. 2nd edition. London: Academic Press.Hinchliff CE, Smith SA, Allman JF, Burleigh JG, Chaudhary R, Coghill LM,

23 Oct 2023: Indeed, withk = t, we have:. Euler: un1 = (I kA)un, ez = 1 z O(z2);Implicit Euler: un1 = (I kA)1un, ez = (1 z)1 O(z2);.

4 Jan 2024: Ex = ωA sin(nπy. a. ). sin(kz ωt). and. By = kA sin(nπy.

20 Apr 2024: automatically patched at x = a as well. We have. (x) cts at x = a ) B cos ka = Aea. ... plot the graph = k tan ka in blue, and then superpose this with the circle.

7 Apr 2021: m!2 = 2 eika eika. = 4sin2. ka. 2. We find the dispersion relation! = ... 2 =. mM. hm M. p(m M)2 4mM cos2(ka). i. The resulting dispersion relation is sketched in Figure 74 in the first Brillouin zone.