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

2 Jul 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.

2 Jul 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.

26 Jun 2024: Quantum Mechanics. David Tong. Department of Applied Mathematics and Theoretical Physics,. Centre for Mathematical Sciences,. Wilberforce Road,. Cambridge, CB3 OBA, UK. http://www.damtp.cam.ac.uk/user/tong/quantum.html. d.tong@damtp.cam.ac.uk.

2 Jul 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.

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

10 Apr 2011: 3). vs T = - l/Ka• Recall that this expression refers to the formulation in Eq. ... I(K1,K2 ,Ka) =! Ko+ In Tria,) exp[L: Keff(l- Oa,a /)] , (lJ) (16).

2 Jul 2024: T Ma, KA Verchand, RJ Samworth. (2024). (link to publication). Deep Block Proximal Linearised Minimisation Algorithm for Non-convex Inverse Problems.

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

2 Jul 2024: T Ma, KA Verchand, RJ Samworth. (2024). (link to publication). Reconstruction of rough surfaces from a single receiver at grazing angle.

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

2 Jul 2024: T Ma, KA Verchand, RJ Samworth. (2024). (link to publication). A new computational framework for log-concave density estimation.

2 Jul 2024: Dynamics of migrating sand dunes interacting with obstacles. KA Bacik, P Canizares, CCP Caulfield, MJ Williams, NM Vriend. – ... KA Bacik, C-CP Caulfield, NM Vriend. – Phys Rev Lett. (2021).

2 Jul 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. –

2 Jul 2024: KA Bacik, P Canizares, CCP Caulfield, MJ Williams, NM Vriend. – Physical Review Fluids. ... KA Bacik, C-CP Caulfield, NM Vriend. – Phys Rev Lett. (2021).

2 Jul 2024: SS AbdusSalam, BC Allanach, HK Dreiner, J Ellis, U Ellwanger, J Gunion, S Heinemeyer, M Kramer, 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

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

2 Jul 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,

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

2 Jul 2024: KA Mizerski, K Bajer, HK Moffatt. – Journal of Fluid Mechanics.

2 Jul 2024: E Sanz, KA White, PS Clegg, ME Cates. – Phys Rev Lett.

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

2 Jul 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

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.

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! =

8 Nov 2017: a r t i c l e’s s u r f a c e τ τ ζ θ ζ ξ ζ = C kA D/ ( ) ( , ) (1 ) /0.

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

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,

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.

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.

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);.

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

2 Jul 2024: G Del Zanna, KA Berrington, HE Mason. – Astronomy & Astrophysics.

26 Jul 2013: FIG. 4. (Color online) Instantaneous velocity and pressure fields (left) and z component of the vorticity (right) for the in-plane beating oftwo flagella, with ka = kb = 0.05, R = 1, ... Bottom: Variation of the ratio of the minimum to themaximum of the

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

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.

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

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).

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

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.

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).

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.

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

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.

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).

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 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

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.