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10 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.

10 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.

10 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.

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

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

10 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).

10 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,

10 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,

10 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

10 May 2024: SD Bachman, JR Taylor, KA Adams, P Hosegood. – Journal of Physical Oceanography. ... KA Adams, P Hosegood, JR Taylor, JB Sallée, S Bachman, R Torres, M Stamper. –

10 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).

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

10 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,

10 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

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

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.

10 May 2024: Domiciliary thrombolysis by general practitioners [2]. AC Pell, KA Fox. – The BMJ.

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

10 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

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

10 May 2024: KA James, PV Landshoff. – Physics Letters B. (1990). 251,. 167.

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

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

10 May 2024: KA Bacik, S Lovett, C-CP Caulfield, NM Vriend. – Physical Review Letters.

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

10 May 2024: KA Bacik, S Lovett, C-CP Caulfield, NM Vriend. – Physical Review Letters.

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.

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

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

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.

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.

16 Apr 2020: SCS =ÿ. a=R,I. ka. 24fi2. Aa dAa dAa (3.4). There can also be mixed Chern–Simons terms which we will discuss later in this sub-section.

15 Apr 2021: Field Theory in Cosmology (Part III). Enrico Pajer. Contents. 1 A quick review of background cosmology 51.1 Classical cosmological backgrounds. 51.2 Motivations for Inflation. 101.3 A prolonged phase of quasi-de Sitter expansion. 151.4 Single field

29 May 2017: GO. RAN. KA. POR. / A. LAM. Y ST. OC. K PH.

3 Mar 2020: 1.3 Time-independence. Definition. A spacetime is stationary if it admits a Killing vector field ka whichis everywhere timelike: gabk. ... akb < 0. We can choose coordinates as follows. Pick a hypersurface Σ nowhere tangentto ka and introduce

8 Apr 2008: Plugging. into the equation we find c = kaa0kbka. for kb 6= ka.

30 Sep 2008: ii) χ(a) = 0 A sin(ka) = 0 ka = nπ where n = 1, 2,. ... Imposing continuity of χ(x) at x = a gives,. A cos(ka) = D exp(κa) (35).

29 Jul 2007: Ka = αAβ̂A′ α̂AβA′ is a Killing vector, and deduce the form of themetric.

1 May 2020: Ka|p〉 = 0. (7)The n-th order ‘descendents’ of the primary are defined by acting on theprimary with n momentum operators:.

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

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

27 Jul 2012: Thus we find. 2χei = Yi Ui iβjUj 12 (Vij Sij )βj θai ka. = ... ka 2δ4(x) , (3.35b)〈. Tρρ(x)Tµν (0)〉. 〈Θ(x)Tµν (0). 〉= 13 (2d τ.

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.

24 Dec 2014: Emacs Lisp List. Last updated: Wed Dec 24 11:36:00 2014. 1270 entries. Mail me (sje30@cam.ac.uk) with any suggestions for changes to this list. View recent changes to the list. 2013-06-07. I am no longer actively updating the list, as I hope that

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

1 Sep 2011: On Lp-boundedness of the L2-projectoronto nite element spacesA. Yu. Shadrin1. IntroductionIn [Sh] we proved that, for p suciently close to 2, the Lp-norm of the L2-projector P onto the space S of polynomial splines of order k on a knot-sequence is