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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.

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.

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.

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

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,

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.

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

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.

28 Aug 2019: 3.24). since t, being the upper limit of the integral, is the latest time so HI(t) can be pulled. ... For n = 4,. the equation reads. T(1234) = : 1234 : z}|{12 : 34 :. z}|{13 : 24 : four similar terms. z}|{12. z}|{34. z}|{13. z}|{24.

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

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).

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

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

19 Jul 2019: Vanadium with Z = 23 has electron configuration. [Ar]3d34s2, but it is followed by chromium with Z = 24 which has [Ar]3d54s1. ... singlet (7.22) which we write as. |ab; s = 0i = ab,(r1, r2) |0, 0i (7.24).

30 Nov 2019: P ψ = ψ ⟨v,ψ⟩v. (2.24). These equations have initial conditions α(0) and η(0,r) such that. ... ˙̃η1 = η̃2 O3(A,η̃), ˙̃η2 = Lη̃1 O3(A,η̃). (2.27). 24 The φ4 kink on a wormhole spacetime.

19 Jul 2019: Z x. a. dx0p2m(E V (x0)). 4. (6.24). Note the minus sign in the phase shift /4. ... 4. (6.25). We’re left with two expressions (6.24) and (6.25) for the wavefunction in Region 2.

23 Nov 2019: ijkSk [Si, S2] = 0. (5.24). as well as [Si,Lj] = 0.

17 Sep 2019: rotator andliquid phases [24].

22 Jan 2019: Un(0)=3Q. 2(2n1)(2n1)(2n3). δn1Q. 23. , (2.20). Un(τb) = 3Q. 24(2n1). [e(n3/2)|τb|. ... 2.24). Projecting these two equations along P′n(µ), and using (2.14)–(2.16) leads to.

8 Dec 2019: cy. I. 1cIδγMa. Bi Peχk. g. 1Bi Peχ. δ. (3.24). 3.3. ... and dΓ /dx|x0 γMa. For the lastterm, we use (3.24) to scale the integral.

17 Jun 2019: 0. (4.24). in order to advect Q. C. S. or 1=Q. ... physical space can be obtained from (4.14). Thus equations (4.16), (4.21) and (4.24), with (4.14), express in a remark-.

22 Jul 2019: s = a zc = a(1. 1 24&24&. )= a. 2e 0.24a, (21). ... Ras,bl =g(R a)Δ#.3s. "%s0= 14&. 2. 2eKT, (24). and hence an expression for the critical thickness of the crustal boundary layer,.

26 Nov 2019: 24). The computational effectiveness of these equations has been demonstrated [107]by tackling small size Ising type problems of order up to 20. ... A variety of potential landscapes to confinepolariton or photons have also been engineered [96, 4, 24].

19 Jul 2019: 9. Quantum Foundations. What is the essence of quantum mechanics? What makes the quantum world truly. dierent from the classical one? Is it the discrete spectrum of energy levels? Or the. inherent lack of determinism? The purpose of this chapter is

24 Jan 2019: January 24, 2019. Abstract. Orthogonal systems in L2(R), once implemented in spectral methods, enjoy anumber of important advantages if their differentiation matrix is skew-symmetricand highly structured. ... 5, Oliver & Boyd. 24. Bader, P., Iserles, A.,

6 Feb 2019: 24. Malmquist, F. (1926), Sur la détermination dune classe de fonctions analytiques parleurs valeurs dans un ensemble donné de poits, in ‘C.R.

19 Jul 2019: r(10.24). The 1/r fall-o follows from solving the free Schrödinger equation; we’ll see this ex-.

27 Apr 2019: It is well known that the singular behaviour can be predicted from the geometry of the domain[22–24]. ... Fn(z) = 2nn!D(22n)(z). (3.24)Both of these (as well as their derivatives) have well-known recursion relations for quick andaccurate computation.