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8 Jan 2018: I. Larkin and Y. N. Ovchinnikov, Sov. Phys. JETP 20, 762. ... Rev. Lett. 72, 2757(1994). [20] H. Shishido, T. Ueda, S. Hashimoto, T.

15 May 2018: width of 110 m. This gives a maximum measurable alti-. tude of around 20 km, although it is typically only used. ... grid spacing below ;20 km (see Tables 2 and 3) and, forhourly data, spatial resolution has little effect below.

30 Apr 2018: Professor Mark Warner. (revised 20.02.18).

20 Mar 2018: Preprint submitted to MPhil in Scientific Computing March 20, 2018. functional theory, configuration interaction etc.). ... Ĥ |ψT〉 = E |ψT〉 (20). Then both the variational and the local energy becometrivial:.

26 Feb 2018: 20. 5.1.1 Varying PminT. 205.1.2 Varying track smearing (σ). 23. 5.2 Increased pileup. ... Figure 20: Reconstruction of vertices by the merge clustering algorithm (with mergedistance set to 0.525mm, using the ‘minimax’ metric) PminT = 1GeV.

26 Feb 2018: 20. 30. 40. 50. 60. 10.4140 10.4150 10.4160 10.4170. Frequency(GHz). Power. ... Frequency(GHz). Power. (nW). 10.4140 10.4150 10.4160 10.417010. 20. 30. 40. 50.

5 Feb 2018: qΔ/10. 2. q1/103. qΔ 0.06(f). 0. 5. 10. 15. 20. 25. ... 5. 10. 15. 20. 0 5 10 15. (E-E. 0)/1. 0-5.

21 Jan 2018: 20 ω. 21). [3]. In the limit k , ω21 and η 0, which in turn gives ω2 = ω20.

23 Jan 2018: Pseudopotentials for a dipolar ultracold atomic gas, Electronic Structure Discussion Group, TCM, University of Cambridge, 18 March 2015; and Quantum Cambridge Winter School, St Hugh's College Oxford, 20-23 March

1 Dec 2018: Stat Comput (2010) 20: 1–7 3. we define the effective sample size by. ... Am. Stat. 52(2), 93–100 (1998). Stat Comput (2010) 20: 1–7 7.

9 Dec 2018: D1plusD2 0 (0) 4 (20) 2 (10) 2 (10) 9 (45) 0 (0) 3 (15) 20. ... Progression free survival (months). 0.8. 1.0. 0 20. Pre–BI, n = 3/5.

3 Oct 2018: Pp(AB) Pp(A) Pp(B). Remark 1.20. FKG stands for Fortuin, Kasteleyn and Ginibre. ... We now prove (1.20). First of all we note that for all n 1.

21 Nov 2018: Theorem 1.1 (Cutoff for Full System). For all λ > 1, all ε (0, 1), all M N and all n sufficientlylarge, for p = λ/n and µ (log ... 0, 1}E with πER(H) = 1 o(1) so that,for all η0 H, for µ (log n)20/n, we have.

3 Oct 2018: P =. . . . . . 1. 20 0 0 1. ... 4. 1. 4. 1. 4. 1. 41. 20 0 0 1.

24 Apr 2018: Geoffrey Grimmett, Zhongyang Li. European Journal of Combinatorics 20 (2013), Paper P47, 14 pp.

11 Sep 2018: 20 GRIMMETT AND LI. In this section, we discuss the bridge constant for transitive graphs,therein introducing the graph height functions that will be useful inthe discussion of locality in Section

21 Feb 2018: 2017. Composition of the European Parliament – The FPS-Method. Typescript, 20 August 2017 (www.uni-augsburg.de/pukelsheim/2017Brussels/). ... 205–20. SŁOMCZYŃSKI, WOJCIECH and KAROL ŻYCZKOWSKI. 2012. Mathematical aspects of degressive

14 Jul 2018: We pick w πm such that. 20 GEOFFREY R. GRIMMETT AND ZHONGYANG LI. ... J. Combin. 20 (2013), Paper P47.[16] , Strict inequalities for connective constants of regular graphs, SIAM J.

4 Jan 2018: We shall show that. (1.20)n. j=1ivj ,vj1 = 0,. and this will confirm (1.12), on recalling that we = 1 for all e E. ... 0 otherwise. Therefore, B makes a contribution towards the sum in (1.20) that is equal toN1(F+F), where F+ (respectively, F) is the

27 Aug 2018: Keren Carss 1, Juan Pablo Casas. 3,20, John C. Chambers. ... 58Department of Quantitative Social Science, UCL Institute of Education, University College London, 20 Bedford Way, London WC1H 0AL.

17 Jul 2018: FOR PHASE M23C6:20:3:6 SIMPLIFIED MODEL USED FOR PHASE TI2N:2:1 SIMPLIFIED MODEL USED FOR PHASE FE2U:2:1 SIMPLIFIED MODEL USED FOR PHASE FESB:1:1 SIMPLIFIED ... ABSENT CHEMICAL ORDERING(C) 18 FCC_L12 ABSENT CHEMICAL ORDERING 19 M23C6 NORMAL PURE

15 Jan 2018: krisnnaswamy S.V. ano Muller S.J. 1973 20 Rield JlSSlOn Symvosium. Penn State Univ., Pa.Krishnaswamy S.V. ... W). '20. 1970 ”“ys Shot. So] (0) 1 513Rev. Lett._Z 911.

16 Jan 2018: Fourmodel alloys were chosen from the systems nickel-aluminium. (Ni—14.1at.%Al), nickel—chromium-aluminium (Ni-20.0at.%Cr-1U.Oat.%Al).

9 Mar 2018: creep strength; whilst the small difference (20 C) in ageing temperatures had significant impact. ... under development [17-20]. However, the combination of the Laves phases and β-NiAl.

20 Nov 2018: 19. 20. Impossible to avoid partitioning substitutional solutes if local equilibrium is demanded. ... Current Opinion in Solid State and Materials Science,. 20 (2016) 396-400.

3 Oct 2018: ARTICLE HISTORYReceived 15 April 2018Revised 18 April 2018Accepted 20 April 2018.

26 Jul 2018: Acta Metall.1953;1:22–31. [20] Robert AY. The Rietveld Method. Oxford: Oxford Uni-versity Press; 1993. ... 2013;84:20–30. [42] Zamberger S, Kozeschnik E. Carbo-nitride precipi-tation in tempered martensite - computer simula-tion and experiment.

26 Jul 2018: 57 2.5 1.52 3.20 0.46F22 0.12 0.35 2.20 0.93 – 0.003. ... 20] Bhadeshia HKDH, Svensson L-E. Modelling the evolu-tion of microstructure in steel weld metals.

16 Oct 2018: condition and was machined into 20 1 65 mmcoupons before being hardened to a martensitic con-dition. ... The heating rate chosen for this investiga-tive experiment is 10, 20, 50, 100C h1.

17 Jan 2018: Schaeffler Technolo-gies GmbH & Co. KG. 17.20-17.45. Bainitic transformation and combination process. ... 09.20-09.45. Process technology and plant design for austempering. Dr.-Ing. Herwig Altena.

3 Apr 2018: These waveletswere applied in a sliding window with 20-msec incrementsin the 0–2000 msec interval.

6 Dec 2018: pants underwent a free recall phase and then a cued recall phase for eachautobiographical memory, lasting 20 min in total. ... probabilisticanatomical cranio-cerebral correlation via the international 10 –20 sys-tem oriented for transcranial functional

12 Nov 2018: Meeting concluded 20.13. Respectively submitted by,. Aime Rankin. MCR Secretary.

12 Nov 2018: Meeting concluded 20.33. Respectively submitted by,. Aime Rankin. MCR Secretary.

12 Nov 2018: Creation of a new Committee position: Ethnic Minorities Officer. The survey for the creation of the new committee position received 20 responses, 12 of which.

12 Apr 2018: 20]. These studies have only used a limited number of hosts, and so do not provide informa-. ... evidence that these changes are adaptive [20]. We then examined whether these same genetic.

31 Dec 2018: Zvib =1. 2. Zddpe. Hvib =kBT! (2.20). The average vibrational energy of each molecule is now.

31 Dec 2018: Unfortunately, the integrals (3.20) and (3.21) look pretty fierce. Shortly, we will start. ... this section if you’re impatient). Let’s look at the particle density (3.20),.

31 Dec 2018: G = F pV = E pV TS (4.20). This is a Legendre transform of F , this time swapping volume for pressure: G = G(T, p). ... already seen in Section 1.4.1. From its definition (4.20), we see that the Gibbs free. –

30 May 2018: 20] Holographic Q-Lattices. JHEP 1404 (2014) 040 arXiv:1311.3292 [hep-th]. Aristos Donos and Jerome Gauntlett.

26 Apr 2018: Thisis. asupe. rvisor’s. copy. oftheno. tes. Pleasedo. notdistribu. teto. stud. ents. Mathematical Tripos: IA/IB Computational Projects. Contents. 0 Introduction 1. 0.1 Overview. 1. 0.2 Aims. 1. 0.2.1 Understanding algorithms. 2. 0.2.2 Being able

8 Jan 2018: diameters) long with t = 0, 0.25, 0.5, 1, 2.5, 5, 10, 20 and Topt = 29.35 D/U (going downwards: flowis from left to right) where U is ... Red dots indicate thetimes (t = 0, 20, 60 and 100) where cross-sections of the total flow (left: 8 contours across [1

23 May 2018: Iserles (ed.), Acta Numerica 20, Cambridge Univ. Press (2011). A. Iserles (ed.), Acta Numerica 19, Cambridge Univ.

2 Nov 2018: 3.20). On the other hand, if m and n go to infinity in case (6), we consider the expression. ... 20. Figure 3.3: log10 |dm,n| (the blue dotted line) and its asymptotic approximation (thered line), for n = 0 (the top left), m = 0 (the top right), m = n

21 Apr 2018: 60. 40. 20. 0. time. Laser profile. e1(t). 4 2 0 2 4.

17 Apr 2018: measuredµ(ξ) = |ξ|2ηeξ. 2. dξ, ξ R. 20. They obey the three-term recurrence relation.

3 Apr 2018: O(h4)︷ ︸︸ ︷iΛ [ψ]1,1(h) 2i. 〈2xµ2,1(h). 〉2, (2.20). whereψ(h,ζ,ξ) = ζ ξ h3. ... Magnus–Lanczos. In Figure 4.3 (right) and Figure 4.4 (right) we show the errorsin exponentiating the order six Magnus expansions (with and without

13 Dec 2018: 20). where Xl = 12 (xl1 xl). The last subintegral with singularitycan be approximated by. ... Then everything turns to be knownin Eq. (20) except the discrete ψ′(Xl).

13 Dec 2018: For example, without further approximation,evaluation for a scatterer of around 220 by 20 wavelengthscan be carried out in around 100 minutes using 32processors on the SunFire machine. ... 0.05 0.05 0.2 0.6 1.0 1.4 1.8. Fig. 1 Surface current amplitudes

13 Dec 2018: allows derivation of analytical results [17–20]. ... 20. M. Spivack, Solution of the inverse scattering problem for grazing incidence upon a rough surface,J.