Search

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.

29 Nov 2018: 7.1). n2/5{f̂n(x0) f0(x0)}. d(. f0(x0)3|φ′′0 (x0)|24. )1/5H ′′(0),. where {H (t) : t R} is the “lower invelope” processof Y , so

9 Dec 2018: Myeloma IX 1 (0) 14 (6) 23 (9) 59 (24) 105 (43) 8 (3) 37 (15) 247. ... Stage II 1 (0) 18 (7) 25 (9) 65 (24) 105 (39) 15 (6) 39 (15) 268.

3 Oct 2018: 21. 1.9 Power law inequalities at the critical point. 24. 1.10 Grimmett Marstrand theorem. ... This is exactly what the BK inequality says. Definition 1.24. For every ω = {0, 1}E and a subset S E we write. [

21 Nov 2018: Cutoff for Random Walk on Dynamical Erdős-Rényi Graph. Perla Sousi Sam Thomas. Abstract. We consider dynamical percolation on the complete graph Kn, where each edge refreshes itsstate at rate µ 1/n, and is then declared open with probability p =

24 Apr 2018: Geoffrey Grimmett and Zhongyang Li. The Electronic Journal of Combinatorics 24 (2107) paper P4.38. ... Julien Berestycki, Nathanael Berestycki, Vlada Limic. Ann. Appl. Probab. 24 (2014) 449–475.

11 Sep 2018: SELF-AVOIDING WALKS 11. The proof follows quickly by earlier results of Woess [73], and Gilchand Müller [24]. ... By [73, Thm 11.6], every G G,g is covered by F ,and by [24, Thm 3.3], F has connective constant 1/ζ.

14 Jul 2018: The planof the proof is as in [24], but the details are more complicated. ... Soc. B 16 (1954),23–38. [24] J. M. Hammersley and D. J.

4 Jan 2018: By (1.23) and(1.24), |i(n)|= 1/Reff(n). The theorem is proved on noting that. ... rimm. ett. 24 Uniform Spanning Tree. 4. Iterate the above process, by running - .

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,.