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3 May 2024: KA Hogan, KLP Warburton, AGC Graham, JA Neufeld, DR Hewitt, JA Dowdeswell, RD Larter. – ... KA Hogan, KLP Warburton, AGC Graham, JA Neufeld, DR Hewitt, JA Dowdeswell, RD Larter.

3 May 2024: KA Hogan, KLP Warburton, AGC Graham, JA Neufeld, DR Hewitt, JA Dowdeswell, RD Larter. – ... KA Hogan, KLP Warburton, AGC Graham, JA Neufeld, DR Hewitt, JA Dowdeswell, RD Larter.

3 May 2024: KA Hogan, KLP Warburton, AGC Graham, JA Neufeld, DR Hewitt, JA Dowdeswell, RD Larter. – ... KA Hogan, KLP Warburton, AGC Graham, JA Neufeld, DR Hewitt, JA Dowdeswell, RD Larter.

3 May 2024: KA Roehrig, D Skinner. – Journal of High Energy Physics. (2018).

3 May 2024: A Atoufi, KA Scott, ML Waite. – Physical Review Fluids. (2020).

3 May 2024: KA Bacik, P Canizares, CCP Caulfield, MJ Williams, NM Vriend. – Physical Review Fluids. ... KA Bacik, C-CP Caulfield, NM Vriend. – Physical Review Letters. (2021).

3 May 2024: MJ West, DB Seaton, DB Wexler, JC Raymond, G Del Zanna, YJ Rivera, AR Kobelski, B Chen, C DeForest, L Golub, A Caspi, CR Gilly, JE Kooi, KA Meyer, BL Alterman,

3 May 2024: DeForest, L Golub, A Caspi, CR Gilly, JE Kooi, KA Meyer, BL Alterman, N Alzate, V Andretta, F Auchère, D Banerjee, D Berghmans, P Chamberlin, LP Chitta, C Downs, S Giordano,

3 May 2024: KA Bacik, P Canizares, CCP Caulfield, MJ Williams, NM Vriend. – Physical Review Fluids. ... KA Bacik, C-CP Caulfield, NM Vriend. – Physical Review Letters. (2021).

3 May 2024: KA Roehrig, D Skinner. – Journal of High Energy Physics. (2018).

3 May 2024: MJ West, DB Seaton, DB Wexler, JC Raymond, G Del Zanna, YJ Rivera, AR Kobelski, B Chen, C DeForest, L Golub, A Caspi, CR Gilly, JE Kooi, KA Meyer, BL Alterman,

3 May 2024: SS Abdussalam, BC Allanach, HK Dreiner, J Ellis, U Ellwanger, J Gunion, S Heinemeyer, M Krämer, M Mangano, KA Olive, S Rogerson, L Roszkowski, M Schlaffer, G Weiglein. – ... SS AbdusSalam, BC Allanach, HK Dreiner, J Ellis, U Ellwanger, J Gunion, S

3 May 2024: R Hložek, AI Malz, KA Ponder, M Dai, G Narayan, EEO Ishida, TA AllamJr, A Bahmanyar, X Bi, R Biswas, K Boone, S Chen, N Du, A Erdem, L Galbany, A

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.

3 May 2024: S Hild, D Hoak, KA Hodge, D Hofman, K Holt, P Hopkins, T Horrom, D Hoske, DJ Hosken, J Hough, EJ Howell, Y Hu, E Huerta, B Hughey, S Husa, SH ... B Sorazu, T Souradeep, A Staley, J Stebbins, M Steinke, J Steinlechner, S Steinlechner, BC Stephens, S

3 May 2024: 1015. (doi: 10.1136/bmj.305.6860.1015). Domiciliary thrombolysis by general practitioners [2]. AC Pell, KA Fox. –

3 May 2024: KA Mizerski, HK Moffatt. – Geophysical and Astrophysical Fluid Dynamics. (2018).

3 May 2024: SD Bachman, JR Taylor, KA Adams, P Hosegood. – Journal of Physical Oceanography.

3 May 2024: E Sanz, KA White, PS Clegg, ME Cates. – Physical review letters.

3 May 2024: A gluing operator for the ambitwistor string. KA Roehrig, D Skinner. –

3 May 2024: van Leeuwen KA, G Oppen, S Renwick, JB Bowlin, PM Koch, RV Jensen, O Rath, D Richards, JG Leopold. –

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.

3 May 2024: S Babak, JG Baker, MJ Benacquista, NJ Cornish, SL Larson, I Mandel, ST McWilliams, A Petiteau, EK Porter, EL Robinson, M Vallisneri, A Vecchio, M Adams, KA Arnaud, A Blaut, M

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.

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);.

20 Sep 2011: ω 6= 0 so ω defines a Killing vector Ka.Killing identity Ka RabKb = 0, where Rab = gab/4. ... M|K|2gd4x = 1. 4. M|K|2gd4x. Therefore Ka = 0 and our assumption was wrong.

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

18 Sep 2022: q. kA(eiqa/2 eiqa/2). Notice that only the combination (r t) appears.

23 Apr 2021: q. kA(eiqa/2 eiqa/2). Notice that only the combination (r t) appears.

19 Jul 2019: q. kA(eiqa/2 eiqa/2). Notice that only the combination (r t) appears.

23 Jul 2009: Third, if ka 9 1 then the relevant scale of number-density fluctuations is small compared with the size of an individual particle. ... 1 ) , ( 2. 2 ) ; and for the case ka 4 1 and a general form of P by Batchelor (1983).

17 Nov 2008: The answer is. G = dt2. ka 3 a3 c+. a da2(ka 3 a3 c. ... L = a3. 4L(Z) 3. 8π G(a(ȧ)2 ka), where Z = ψ̇ 2 (4.4).

3 May 2024: van Leeuwen KA, G Oppen, S Renwick, JB Bowlin, PM Koch, RV Jensen, O Rath, D Richards, JG Leopold. –

3 May 2024: MR Bate, SH Lubow, GI Ogilvie, KA Miller. (2003). (doi: 10.48550/arxiv.astro-ph/0301154).

10 Apr 2011: 2 6 ) - ( 2 8 ) to order 1/(Ka) 2 the following expression for the surface potential:. ... 1 2 ( q - 1) 1 ( q - 1)2(2q 1) 3 3 , (29) = 2 l n ( p q) Ka p q ( K a ) 2 p q.

3 May 2024: KA Adams, P Hosegood, JR Taylor, JB Sallée, S Bachman, R Torres, M Stamper. –

19 Jul 2019: 2=. mM. hm M. p(m M)2 4mM cos2(ka). i. The resulting dispersion relation is sketched in Figure 57 in the first Brillouin zone. ... This is because it is. valid only at long wavelengths, ka 1.

10 Apr 2011: Trapping and Wiggling: Elastohydrodynamics of Driven Microfilaments. Chris H. Wiggins, D. Riveline,# A. Ott,# and Raymond E. Goldstein. Department of Physics, Princeton University, Princeton, New Jersey 08544 USA; #Institut Curie, Section de

16 Apr 2021: na=1. La〈O(k1)O(k2). O(kn)〉 = 0 , (1.1). where La = L(τa,τa, ka,ka) is some linear, possibly differential operator made of func-. ... Then (4.26) becomes[. 3(n 1) na=1. ka. ka. ]〈R(k1)R(k2). R(kn)〉′! = 0 , (4.38).

15 Apr 2021: φ(k1). φ(kn)〉 δ3D. (na=1. ka. ). (19). 7. For the metric. ... φ(k1). φ(kn)〉 = (2π)3δ3D. (na=1. ka. )Bn(k1,. ,kn). (34). must scale as.

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 64 in the first Brillouin zone.

8 Mar 2012: This gives. Aκ cos κa. A sin κa=. B k cos (ka δ0). ... γl =κaj′l(κa). jl(κa). (4.1.2.2). As k 0 have γl const, jl(ka) (ka)l, nl(ka) (ka)(l1) and, as before, getδl (ka)2l1.

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.

19 Oct 2013: #"$ %'&)(,.-0/$1#(23547684:9 ;8< = >?9A@B9DCFE7;8<G9IH 4KJ L59NM. OPRQST U U U U V W XY XY X X X XZ XY XY X. X XU XU. [#[T U U U U]_)]_)a.bc)_edXU XZ X X XZ X X XU XZ X f b)ghd. XZ X XZ X X Xi. [)jT U U U Uk]_l]DmBnoDdXi Xi XZ XU XZ X XU XZ XZ XZ X

10 Apr 2011: Trapping and Wiggling: Elastohydrodynamics of Driven Microfilaments. Chris H. Wiggins, D. Riveline,# A. Ott,# and Raymond E. Goldstein. Department of Physics, Princeton University, Princeton, New Jersey 08544 USA; #Institut Curie, Section de

26 Jul 2013: with similar viscosities (, ) and densities (, ),(b) dimensionless membrane-viscous number, Me U=KA, for two fluids separated by an elastic membrane(thickness t, area modulus KA, density m, bending stiff-ness ... f 2= is an intrinsic viscocapillary

12 Mar 2015: components are. Ex = ωA sin(nπy. a. )sin(kz ωt). By = kA sin(nπy.

18 Oct 2019: non-negative, because. n = nhn|ni = hn|N |ni = hn|A†A|ni = kA|nik2 0 (3.11). ... Taking the norm of both sides shows that. |cn|2 = kA†|nik2 = hn|AA†|ni = hn|N 1|ni = n 1.

20 Jan 2011: 2.12)Consider a complex tetrad of 1-forms. Ka = i(α̂AβA′ αAβ̂A′ ), Xa = α̂AβA′ αAβ̂A′ , Za = αAβA′. ... We now use(2.16) to find. φAB = 2|K|2 KA′B AA′. (1.

20 Jan 2009: Ex = ωA sin[ nπy. b. ]. sin(kz ωt),. By = kA sin[ nπy.