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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).

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.

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.

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

22 Jan 2019: Production of programmable self-folding films at microscalecan be achieved via patterning of multiple layers with different swell-ing properties (22–24) or creation of spatial concentration gradients(25, 26). ... Adv. Mater. 27, 79–85 (2015). 24. M. Z

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

19 Jul 2019: ai bj = 2 ij (2.24)? is sometimes referred to as the dual lattice. ... 53 –. The condition (2.24) can also be stated as the requirement that.

5 Nov 2019: In recent modeling work involving locomotion of bacteriaand spermatozoa, boundary integral equations for the cellbody combined with slender-body theory for the flagellumhave proved to be accurate and efficient [23,24]. ... 24] D. J. Smith, E. A. Gaffney,

30 Dec 2019: Let (M,g) be an ASD Einstein manifold with scalar curvature 24 admitting a parallel ASD totally nulldistribution.

14 Nov 2019: Chem. Soc. 2001,. 123, 11284.[24] C. E. Reese, A. V. Mikhonin, M.

23 Nov 2019: c2v E = 1. µc2p. (er̂. 4π0r2. )= e. 4π0µc21. r3L (8.24). ... The first ionisationenergy is thus the difference (54.4 79.0) eV = 24.6 eV.

6 May 2019: The deflection reduces to the classic bell-shaped form [23,24]. h(r ) = p̃R4F. ... Masse, Laboratory experiments in fracture propagation, Soc. Petr. Eng. J. 24, 256(1984).

28 Aug 2019: 4.23). S[] = exp12 S. (4.24). Although the basis of generators M and S are dierent, we use the same sixnumbers in both and S[]: this ensures that we’re

15 Aug 2019: anm0:. 0.30:. 0.29:. 0.28:. 0.27:. 0.26:. 0.25:. 0.24:. 0.23:. 0.22:. 0.21:.

19 Jul 2019: The anti-. unitary operator acts on angular momentum as (5.24),. L1 = L. ... P2(t) 2. 2sin2. t. 2. (8.24). Electric Dipoles vs Magnetic Dipoles.

23 Nov 2019: Similarly,. |1, 0〉H =12. (|x〉e |x〉p |x〉e |x〉p) (6.24). as one can check straightforwardly.

21 Aug 2019: J. Amer. Math. Soc., 24(1):81–124, 2011. Matthew Colbrook, Bogdan Roman, and Anders Hansen.

27 May 2019: DNA [24,25], spirochaetes [26,27], spiro-plasma [28], trypanosoma [29], and bacterial flagellar fil-aments [17], all take the shape of helices and spirals, asillustrated in Figs. ... 24). 053107-4. PROPULSION BY STIFF ELASTIC FILAMENTS … PHYSICAL