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8 Jan 2018: The effect of Pauli blocking has been carefully analyzed[22–24] for the product of two (N,N) = (1,1) instabilities,and found to give only a small correction to the ... B81, 174514 (2010). [23] W. V. Pogosov and M. Combescot, Physica C 471, 566

15 May 2018: 1976) proposed parameterizations of wind variability. over a range of time periods up to 24 h,.

20 Mar 2018: Eb =1. Nb. RBb. EL(R) (24). 3.2. ImplementationThe following VQMC calculations are carried out us-. ... Beryllium 4 -14.32830 -14.66735 [7]Boron 5 -23.42837 -24.65393 [8]. The calculated variational energies (EV ) of a succession of atomicsystems.

26 Feb 2018: 23. Figure 24: Reconstruction of vertices by the DBSCAN clustering algorithm (with =0.16875mm and minPoints = 2) PminT = 3GeV, σ = 0.1mm. ... 24. Figure 26: Reconstruction of vertices by the merge clustering algorithm (with mergedistance set to 0.525mm,

26 Feb 2018: 24). We see that the term proportional to σ̂↠corresponds. to exiting both the qubit and the cavity.

5 Feb 2018: 3045. 00.410.811.2. xy. g(r. ). (b) (c). 0 12 24 36 012. ... 2436. 00.51. 11.5. 0 12 24 36 012. 2436. 00.51. 11.5.

27 Aug 2018: 24, Sebahattin Cirak. 19,25, Peter Clapham. 1,. Gail Clement26. , Guy Coates1, Massimiliano Cocca. ... Jim Stalker1, Elizabeth Stevens. 19, Jianping Sun. 24,51, Gabriela. Surdulescu26. ,

17 Jul 2018: quit paging : q 22 ORTHORHOMBIC_A20 NORMAL PURE SUBSTANCE 23 TETRAGONAL_U NORMAL PURE SUBSTANCE 24 FE2U NORMAL PURE SUBSTANCE 25 FESB NORMAL PURE SUBSTANCE 26 FEU6 NORMAL PURE SUBSTANCE 27 ... quit paging : q 22 ORTHORHOMBIC_A20 ABSENT PURE SUBSTANCE 23

9 Mar 2018: Nanolab 600 SEM following the standard lift-out procedure [24]. A protective layer of platinum. ... 24. of the primary Laves phase precipitate are substantially lower than those of the secondary ones.

26 Jul 2018: Table 4. ChemicalcompositionoftheprecipitatesandmatrixidentifiedinFigure8.Thesamplewasslow-cooledfromaustenitisationand tempering at 600C for 24 h. Element (wt-%) Ratio. ... Metall Trans.1972;3:2895–2903. [24] Yoo CH, Lee HM, Chan JW, et al.

26 Jul 2018: Austenitising 850 2–6Tempering 575 2–24Tempering 600 1–24Tempering 625 1–24. of 10 ml min 1. ... Prevention of hydrogen embrittle-ment in steels. ISIJ Int. 2016;56:24–36. [14] Honeycombe RWK, H.

16 Oct 2018: J Electrochem Soc. 1990;137(6):1703–1706. [24] Song RH, Pyun SI, Oriani R. ... Wear. 1973;24:107–118. [44] Scott D. Rolling contact fatigue. Treatise Mater Sci Tech-nol.

3 Apr 2018: These clusters included the following: left frontalcluster (Channels 33, 24, 26; equivalent to F3, F7, AF7),mid frontal cluster (Channels 19, 11, 4; equivalent to Fz,F1, F2), right frontal cluster

6 Dec 2018: Neuropsychology 24:465– 475. CrossRef Medline. Huang YZ, Edwards MJ, Rounis E, Bhatia KP, Rothwell JC (2005) Thetaburst stimulation of the human motor cortex.

12 Apr 2018: Adaptation of. HIV-1 to its human host. Mol Biol Evol. 2007; 24(8):1853–60. ... 2012; 15(12):1370–7. Epub 2012/08/24. https://doi.org/. 10.1111/j.1461-0248.2012.01858.x PMID: 22913776. 24. Waxman D, Weinert LA, Welch JJ.

31 Dec 2018: f(r) = eU(r) 1 (2.24). This is a nicer expansion parameter.

31 Dec 2018: 23. 1. z. 4p2+. (3.24). The next part’s a little fiddly. ... 1. 1. 2p2. 3N. V+. which we then substitute into (3.24) to get.

31 Dec 2018: V. A. B. Path I. Path II. Figure 24:. underline the meaning of the new symbol d. ... energy gives us,. @S. @V. T. =@p. @T. V. (4.24). The Gibbs free energy gives us.

30 May 2018: David Tong and Kenny Wong. [24] The Holographic Dual of AdS3 x S3 x S3 x S1.

26 Apr 2018: There are also a number of excellent books, and Google returns about 24,300,000 hits for the search‘Matlab introduction’ (up from 13,400,000 hits last year), and about

8 Jan 2018: Nonlinear NonmodalStability Theory. R. R. Kerswell,School of Mathematics, Bristol University, Bristol, U.K., BS8 1TW; email:. R.R.Kerswell@bris.ac.uk. Xxxx. Xxx. Xxx. Xxx. YYYY. AA:1–30. This article’s doi:. 10.1146/((please add article doi)).

25 Oct 2018: Our local environment and theeconomy. Why nature needs to be taken into account in planning andeconomic decisions. Friday 28 September 2018, 12:45 – 17:30at Centre for Mathematical Sciences, Cambridge CB3 0WA. 12:45 Lunch13:30 Introductory talks

23 May 2018: Iserles (ed.), Acta Numerica 24, Cambridge Univ. Press (2015). A. Iserles (ed.), Acta Numerica 23, Cambridge Univ.

2 Nov 2018: operator (the case γ = 1) represents a challenge for spectral theory (Böttcher, Grudsky &. Iserles 2012). 24. Figure 4.3: The eigenvalues of the integral operator with ω = 100 for γ =

21 Apr 2018: 1Ṽ , (3.4). where V̂ is an O(h3). perturbation of Ṽ ,. V̂ = Ṽ h2. 24 (Ṽ )>(Ṽ ). (3.5). The overall order-four scheme is obtained by substituting the central ... 2. 24 (Ṽ )>(Ṽ )). Thus, a fourth-order compact splitting,. e16 ihε.

17 Apr 2018: 24. (Levin & Lubinsky 2001, Van Assche 2018). Hermite polynomials form the simplestexample, other familiar cases are Q(x) = x4 tx2 for some t R and Q(x) = |x|(whereby smoothness fails

3 Apr 2018: h7), (2.23). Magnus–Lanczos methods with simplified commutators 15. where. ϕ1(h,ζ,ξ) = h2 4hξ 2ζξ, (2.24).

13 Dec 2018: For scalar wave fields witharbitrary incident angles the scattered field obeys the Helmholtzboundary integral equation [1, 24]. ... Sel. Top. Appl. Earth Obs. Remote. Sens. 7,1573–1583 (2014). 24. J.

13 Dec 2018: 24. P. Tran, Calculation of the scattering of electromagnetic waves from a two-dimensional perfectlyconducting surface using the method of ordered multiple interaction, Waves in Random Media, 7,295-302 (1997).

13 Dec 2018: As an illustration of the method, Figure 1 shows comparisons between the firstand second iterations of the operator series with ’exact’ computations from (24 ),restricted to the rough portion of the ... αr r′. = f(r,r′) (24). the expression (23)

13 Dec 2018: h(Xn) = z |Sn(xn Xn)3/2. αφ(Xn)δ|. (24). 2. Medium with Linear Profile. ... Reconstruct the surface h(Xn) by eq. (24) for uniformmedium or (26) for linear profile using Φ obtained aboveend for.

13 Dec 2018: The estuary receives water from a catchment coveringan area of 24,000 km2 and is the largest freshwater supplier to theNorth Sea. ... 0.0. 5.0. 10.0. 15.0. x (km. ). y (km) -30-28-26-24-22-20-18-16-14-12-10-8-6-4-20. 1925 1936.

13 Dec 2018: F′n1, An,n =τ. 2ξF′n. (24). This is easily and rapidly inverted by back-substitution.

13 Dec 2018: and7!:. cr! 5 ESFG r;r8! ]c]z r8!2 ]G]z r;r8!cr8!Gdx8,. 24! where againr85[x8,S(x8)], and S is the union of the sur-facesh1

13 Dec 2018: 0 Zl ( (•(x,zi))=--• Do(X)-- likzi cos 0 --• COS 2 0 eikXx+ h(x)• ,. (24). where • is the variance of the surface height. Here we have neglected an O(a ... 29) Collecting terms, and using (25), (26), and (29), Eq. (24) can now be written. ( {•

13 Dec 2018: T-•=Tg'(1--To •AT Tg:A •. ) (24) so that. E = (2 - 4At 8A•. ... 2. It is easy and computationally inexpensive to take further terms in the se- ries (24).

13 Dec 2018: By (24),〈h(X). I(r). r. 〉=. 〈h(X). d. dr. r0. ikh(r′) cos θeikSr. ′. ... 24] P. Tran, Calculation of the scattering of electromagnetic waves from a two-dimensional per-fectly conducting surface using the method of ordered multiple interaction,

13 Dec 2018: elements. (Bn)mj = Anmnj. (24). We thus require. bn = B1n cn (25). ... from rough surfaces, Waves in Random Media, 6, 151-167 (1996). [24] A.A.

13 Dec 2018: g = (A’ B’)m. where. A’ = a2 -@g. 8’ = -2r [l -! Jtt, $1,! (<, 59 = f(E) f(d. l = @1- 22 - 23 td)/SL, 7 = (21 - 22 2s - 24)/2L, and

13 Dec 2018: 2.1. Formal solution and splitting series. The method of solution is analogous to that applied to the electromagneticproblem in 2-d or 3-d [23, 24]. ... 24] M. Spivack, J. Ogilvy, C. Sillence, Electromagnetic scattering by large com-plex scatterers in 3d,

18 Nov 2018: Doyle and C. McMullen [24]: “But can be solved in the case ofthe quartic and the quintic using several limits (towers of generallyconvergent iterative maps linked serially).”. ... P. Doyle and C. McMullen [24]: “But can be solved in the case ofthe

11 Nov 2018: Amer. Math. Soc., 24(1):81–124, 2011. Introduction Schrödinger and PDEs Discrete operators Numerical Example Conclusion Definitions. ... Solvability Complexity Index (SCI) [24, Hansen, JAMS]. is some set, called the primary set,.

16 Nov 2018: Doyle and C. McMullen [24]: “But can be solved in the case ofthe quartic and the quintic using several limits (towers of generallyconvergent iterative maps linked serially).”. ... P. Doyle and C. McMullen [24]: “But can be solved in the case ofthe

3 Apr 2018: with (2.17).Finally, equation (2.24) is satisfied upon eliminating fww in the sameway and using w. ( ... 24. motion of N-vortices. There are several ways to obtain the metric forboth flat and curved backgrounds [46, 16].

19 Jul 2018: Thus the space oforbits of K2 in MC admits a Toda Einstein–Weyl structure [3, 24].• There exists a combination of self-dual two-forms which is degenerate when the harmonic. ... Roy. Soc. A363 (1978) 289–295.24. R. S. Ward, ‘Einstein-Weyl spaces

10 Mar 2018: A different approach was developed by Painlevé, Kowalevskaya, and Gambier who studied 2ndorder ODEs in the complex domain.16,24. ... Proc. Cambridge Philos. Soc. 156, 99–113. (2014).24 Painlevé, P., “Sur les équations différentielles du

19 Oct 2018: 2.24). Notably, this expression can be simplified into. s0 =sb(rc) r s(.

16 Jul 2018: Phys. Fluids 24, 061901 (2012). 18. Lauga, E. Bacterial hydrodynamics. Annu. ... 24. Johnson, R. E. An improved slender-body theory for Stokes flow.

19 Oct 2018: 14,24,26] The inner sur-face of the cone is chemically active and catalyzes a chemi cal reaction. ... Li, W. Gao, L. Zhang,. J. Wang, ACS Nano 2015, 9, 117.[24] M.

19 Oct 2018: where. T 2X‘. A‘þ1;2ffiffiffiffiffiffiffiffiffiffiffiffiffi2‘þ3p. ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi‘2 þ2‘þ3. 2‘þ1. sM‘2. 24. ‘þ1‘þ2. ... Brown and W. Poon, Soft Matter, 2014, 10, 4016–4027.24