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2 Jun 2019: Re2L =1708. 24[2(1 2)](13). can be made. The minimum of ReL occurs when = 1/4 and is. ... un1 = un J1F(un,Re) (24). where Jij := Fi/uj is the Jacobian and is an NT NT sized complex matrix.

4 Jun 2019: J. Amer. Math. Soc., 24(1):81–124, 2011. [13] K. H. Jin, M. ... In IEEE Symposium on Securityand Privacy, pages 582–597. IEEE, 2016. [24] M.

18 Dec 2019: The predominant approach to this problem has been througha Lagrangian formulation [3, 10], which is the most appropriate for computationalstudies [2, 24, 29, 30]. ... Phys. 203 (2005), no. 2, 539–571. doi:10.1016/j.jcp.2004.08.023. [24] Hou, T. Y.;

30 Oct 2019: 24). This requires B(r) and S(r) to have the same Taylor expansion aroundthe point of interest, r. ... 39). The above integral is the single-layer boundary integral representation for flow around a translatingsphere [24].

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

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.

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.

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

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.

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 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.

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: Pierre Vanhove (IPhT & IHES) D6 R4 Cambridge March 2015 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.

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

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

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.

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