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

29 Jun 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.

29 Jun 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.

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

29 Jun 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.

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

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

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

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! =

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

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

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.

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,

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

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.

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

29 Jun 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).

29 Jun 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. –

29 Jun 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).

29 Jun 2024: Microwave ionization of hydrogen atoms: Experiment vs classical dynamics. van Leeuwen KA, G Oppen, S Renwick, JB Bowlin, PM Koch, RV Jensen, O Rath, D Richards, JG Leopold. –

29 Jun 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

29 Jun 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,

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

29 Jun 2024: KA Mizerski, K Bajer, HK Moffatt. – Journal of Fluid Mechanics.

29 Jun 2024: E Sanz, KA White, PS Clegg, ME Cates. – Physical Review Letters.

29 Jun 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

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

29 Jun 2024: Microwave ionization of hydrogen atoms: Experiment vs classical dynamics. van Leeuwen KA, G Oppen, S Renwick, JB Bowlin, PM Koch, RV Jensen, O Rath, D Richards, JG Leopold. –

29 Jun 2024: G Del Zanna, KA Berrington, HE Mason. – Astronomy & Astrophysics.

29 Jun 2024: KA Bacik, S Lovett, C-CP Caulfield, NM Vriend. – Physical review letters.

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

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.

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.

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).

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.

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.

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

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

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

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.

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.

24 Dec 2014: Emacs Lisp List. Last updated: Wed 24 Dec 2014 11:36:00 GMT. 1270 entries. Return to ELL. c-includes.el --- Find all header files included by a source file. John Wiegley. 2014-11. plimode.el --- [Electric PLI mode: indenting and flashing and filling]

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 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.

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.

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

8 Jul 2021: RESEARCH ARTICLE. The bank of swimming organisms at the. micron scale (BOSO-Micro). Marcos F. Velho Rodrigues1, Maciej LisickiID2, Eric Lauga1. 1 Department of Applied Mathematics and Theoretical Physics, University of Cambridge, Cambridge, United.

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