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6 Feb 2019: Matthias Gaberdiel ETH Zürich. based mainly on. Eurostrings, Cambridge 24 March 2015.

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: δ(BBs) 2.7% 6.6%. δ 24.5% 40.5%. Trento, Beautiful Mesons and Baryons on the Lattice A. ... 1995 ALEPH Λcl 1.02 0.24 0.67 0.16. 1992 ALEPH Λcl 1.12 0.37 0.74 0.24.

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.

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.

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

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.

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.

6 May 2019: h(xF) = h1, (2.11a). h0(xF) = 3h1L. sgd. BL3. 24, (2.11b). ... ĥ =. 24( L̂ x̂)3( x̂) ĥ. ( L̂ x̂)3. L̂3, (2.21).

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

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.

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

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: 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.

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).

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

11 Jul 2019: X12. X34. X24. X13 X14. 23. 21. 12. 32. 14 24.

6 Dec 2019: ca,β ca′,β. (10.24). If the original state |Ψ〉 was simple, so that (say) the ca,β are non–zero only for a singlevalue of β, for which ca, ... However, if |Ψ〉 is a more general, entangledstate then the sum in (10.24) means that ρA is the

11 Jul 2019: D′ψC′D′E′F′ψE′F′. A′B′ , (2.24). which are in general independent. We verify by explicit calculation that if ψABCD and ψA′B′C′D′ arise from ... Proposition 2.3. Let I, J, I′, J′ be the invariants (2.24) of the Weyl