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27 May 2019: Typical curves for the near-field capillaryforce, eqn (24), and the magnetic attraction, eqn (25), areshown in Fig. ... 6c. As expected eqn (25) shows a linear increase. while eqn (24) decreases monotonically allowing for a singlemean separation.

30 Aug 2019: measurements. This gives a non-linear alternative to other methods like generalizedsampling [2, 5, 6, 8, 32, 34, 41] and the Parametrized-Background Data-Weak (PBDW)-method [13, 14, ... This was then further analysed and extended to the PBDW-method by

2 Jun 2019: ν = 0 at boundary, (24). ν = 0. (25). Now, considering variations in u (with the condition that δu = 0 on the boundary): T0. ... Step.3 Backwards time integrate the dual linearized Navier-Stokes equation (35)with incompressibility (25) and boundary

14 Nov 2019: Boundary element methods have long been usedto study problems in bacteria locomotion including flagellarpropulsion,23 interaction between two swimming bacteria,24.

6 Feb 2019: Unquenched calculation. Northwestern University 24 K. K. Seth. Lattice at Trento April 2–6, 2012. ... RBC-UKQCD (2010) 60 8 MeV 24 5 MeV. HPQCD (2012) 70 9 MeV 35 3 MeV.

27 May 2019: Despite these variations, acoherent flagellar bundle is expected to be maintained generically by long-range hydrodynamicinteractions [24,25]. ... 2.24). For a symmetric configuration such that (N. i=1 ω̃(i)t Ri) ez = 0, only the first term of Mprop.

6 Feb 2019: timeL a(fm) ml ms mπ(MeV) # configs. sources. 24 0.11 0.005 0.040 331 1636 124 0.11 0.010 0.040 419 1419 132 0.08 ... EeffBs = 3.1025(12), χ2/dof = 0.41, p = 98% I L = 24.

6 May 2019: 44. 40C. 08:0. 1:4. 07. DD. D 2. 01. 834. 24. ... 01. 834. 24. 4. 530 J. S. Nijjer, D. R. Hewitt and J.

6 Feb 2019: Wang arXiV:1108.2971]. Alexander Khodjamirian Exclusive semileptonic B and Λb decays at large hadronic recoil 24 / 37.

4 Dec 2019: t0〈k||m〉eiωkmt′ dt′ = km. Ek Em(1 eiωkmt. ), (9.24). where km = 〈k||m〉 and ωkm = (Ek Em)/. ... k|†|m〉(ωkm ω). [ei(ωkmω)t 1. ]. (9.32). This is very similar to our result (9.24), with the time–dependence of the perturbation.

20 Oct 2019: 339,. 936–940 (2013). 24. Duan, W. et al. Synthetic nano- and micromachines in analytical chemistry: sensing, migration, capture, delivery and separation.

6 Feb 2019: Pierre Vanhove (IPhT & IHES) D6 R4 Cambridge March 2015 24 / 37.

22 Jul 2019: ic.oup.com/gji/article-abstract/218/1/247/5382046 by U. niversity of Cam. bridge user on 24 June 2019. ... bridge user on 24 June 2019. Evolution of thin-skinned fold-thrust belts 257.

6 Feb 2019: 12 -208 208.455 53252. 15 513 512.958 192401. 23. ATISH DABHOLKAR QUANTUM ENTROPY OF BLACK HOLES 24. •

19 Jul 2019: qg = 2n with n 2 Z (1.24). This is the famous Dirac quantisation condition. ... qg = 2n with n 2 Z. This, of course, is the Dirac quantisation condition (1.24).

6 Feb 2019: O1(x1)O2(x2)O3(x3)O4(x4)〉. =k. λ k12λk. 34@. @k=p. λ p13λp. 24. @. @p.

28 Aug 2019: where µsatisfies. µ. = µ (1.24). For example, a rotation by about the x3-axis, and a boost by v < 1 along the x1-axis. ... transformations. µ= µ! µ. (1.49). where! µis infinitesimal. The condition (1.24) for to be a Lorentz transformation.

10 Apr 2019: Moreover, we have for the transform, that it is linear:. W {af(x) bg(x)} = aW {f(x)} bW {g(x)} a,b R, f,g L2([0, 1]d), ... 5.1 Classical compressed sensing. Compressed sensing was introduced by Candès, Romberg & Tao (19) and Donoho (24)and is

5 Nov 2019: J. 24, 6308–6324 (2018). 24. Moran, J. L. & Posner, J.

6 Feb 2019: 6.2. 6.21. 6.22. 6.23. 6.24. 6.25. 6.26. 6.27. 6.28. 6.29. 6.3.