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30 Sep 2019: Forc. eK. Re. Propulsion at large K. similarityK=100, 200, 400, 1000. ... accele. ration /g. H cos(alpha) /L. Experiments. Grooves 5 heights & 4 lengths, Plates 3 thickness,(K = 0.15 2800, Re = 1 200) a = 0.02 1.4 m/s2.

16 Dec 2019: volume = {820}. year = {2017}. URL = {https://doi.org/10.1017/jfm.2017.200} }.

6 Feb 2019: 0.8. 1. Mat. rix. elem. ent. 0 200 400 600 800Momentum [MeV]. ... 0 200 400 600 800Momentum [MeV]. 1. 0.8. 0.6. Mat. rix.

3 Dec 2019: πr2p = 2πrLσY. Hencep. L= 200 Pa m1. (measure 350 in 100m test).

24 Apr 2019: when n > 13.  For gas molecules in the room d/r 200 leads rapidly to chaos.

3 Dec 2019: πr2p = 2πrLσY. Hencep. L= 200 Pa m1. (measure 350 in 100m test).

6 Feb 2019: b-quark mass computation - 3. µ̄1b. 1/µ̄h (GeV1). y(µ̄. h). 0.800.700.600.500.400.300.200.100.00. ... b-quark mass computation - 4. µ̄1b. 1/µ̄h (GeV1). y(µ̄. h). 0.800.700.600.500.400.300.200.100.00.

6 Feb 2019: HPQCD NRQCD b ’09. Fermilab/MILC ’11. ETMC ’11 (Nf=2). 160 180 200 220 240 260. ... HPQCD ’09. Fermilab/MILC ’11. ETMC ’11 (Nf=2). 120 140 160 180 200 220.

6 Feb 2019: Entries/(0.005GeV). 0. 100. 200. 300. 400. 500. 310. (a). χbJ. (GeV)γ. ... 1S))-M(hadrons) (MeV)Υ M( M -100 -50 0 50 100 150 200 250 300.

6 Feb 2019: 0 5 10 15 200.0. 0.5. 1.0. 1.5. q2 HGeV2L. f2Lb p Hq2L. ... 0 5 10 15 200.0. 0.5. 1.0. 1.5. q2 HGeV2L. g2Lb p Hq2L.

6 Feb 2019: 0 0,05 0,1 0,15 0,2a[fm]. 0. 200. 400. 600. 800. Mπ[. ... 150. 200. 250. 300. 350. 400. Mπ[. MeV. ]CompletedIn productionPlanned. Nf = 211 Hisq MILC ensembles. #

6 Feb 2019: 100 200 300 400D(n,l). 10. 20. 30. 40. 50. 60. Sym20(K3). ... 50 100 150 200 250 300D(n,l). 20. 40. 60. 80. 100.

20 Oct 2019: Short report Physics of Living Systems. 0 200 400 600 800 1000 1200 1400. ... predators. Microbial Ecology 27:189–200. DOI: https://doi.org/10.1007/BF00165817, PMID: 24190275. Gittleson SM, Hotchkiss SK, Valencia FG.

4 Feb 2019: 27, pp. 193-200. Phillips, K. J. H.; Chifor, C.; Dennis, B.

14 Nov 2019: as-prepared size of 5 µm 10 µm 200 µm, which bends and forms a 2D spiral upon swelling in water. ... This property can be understood by examining the dependence of the curvature on the relative strain normalized to the thickness, i.e., ε/h, where ε =

5 Nov 2019: The platinum layercovered almost entirely the nickel binding layer. The scale bar is 200 nm. ... Then the microparticles were baked at 200 C for10 min to solidify the structure.

6 Feb 2019: np. 103 GeV3sinδπ. πnp =. aCP8.2103. Roughly, A()np 10ASM2 hence a > 10-fold enhancement of dnIn fact, rather a factor of 20 to 200. ... c̄σFu: 104 d (SM)nScaled up o2: 10 d. (SM)n. (c̄R uR )(d̄LdL): 200 d(SM)n.

9 Nov 2019: 90 0-40-0-500-80-0-90 0-30-0-400. 70-0-80 0. 20-0-300-60-0-70 0-10-0-200-50-0-60 Below 0.

16 Jul 2019: Short report Physics of Living Systems. 0 200 400 600 800 1000 1200 1400. ... predators. Microbial Ecology 27:189–200. DOI: https://doi.org/10.1007/BF00165817, PMID: 24190275. Gittleson SM, Hotchkiss SK, Valencia FG.

6 Feb 2019: T/k=0.7. T/k=0.9. 0.0 0.5 1.0 1.5 2.00. 200. 400. 600. 800.

14 Nov 2019: U = 1. 1µc(1, µ)dµ =. k13. =14. (22). The series solution for the concentration converges suf-ficiently quickly for a quantitative comparison, howevereven with 200 non-zero coefficients the analytical

14 Feb 2019: How do we address that? The landscape has changed over the last 200 years.

27 May 2019: 0.1. 0.2. 0 0. 0.05. e. 2. 60 300 200 100 0 1000. ... babi. lity. 20. 0 5 10 15 200. 0.02. 0.04. 0.06.

6 May 2019: 1.15. ,. a2/5. ,a>. 1.15. Lu. beet. al. (200. 5). Dry. ... unes. seet. al. (200. 5). Dry. colla. pse. x 1. x ix i. /.

6 May 2019: b,c) Marginal stability curves ( = 0, outlines)and regions of instability ( > 0, shaded areas), for R = 3 and (b) Pe = 25, 200, 500 and(c) Pe = 15, 20, 25.

29 Jan 2019: On the infinite-dimensional QR algorithm. Matthew J. Colbrook† and Anders C. Hansen†. †DAMTP, Centre for Mathematical Sciences, University of Cambridge, Wilberforce Rd,Cambridge CB3 0WA, United Kingdom. Abstract. Spectral computations of

2 May 2019: Resolvent II. Example 3: Back to Graphene. B. 0 200 400 600 800 1000. ... 0. 100. 200. 300. 400. 500. 600. 700. 800. 900. 1000.

6 Feb 2019: Possible solutions:. HQE violated by O(200%3300%) now excluded! Huge new physics in Γ12? - ... Large (O(200 3400%) NP effects in Γ12? Why not seen somewhere else?

6 Feb 2019: excludedregion. 100 200 300 400 500cT.

22 Jul 2019: 32 and (e) t = 200. ... pt/Pe for the same parameters as (b) at t = 200.

6 Feb 2019: bare. 0 50 100 150 200 25010. 8. 6. 4. 2.

22 Jan 2019: For this specific phage,we thus have ah 30 nm, Lt 220 nm, Lfib 200 nm, rfib 1 nm, and Rf l 10 nm. ... II D 1 and Ref. [24]): ah 30 nm, Lt 220 nm, rtail = 7 nm, Lfib 200 nm,rfib 1 nm, Rf l 10 nm, and μ = 103 Pa s.

6 Feb 2019: fB. s. /fB. FNAL/MILC ’11HPQCD ’12. RBC/UKQCD ’10. 180 185 190 195 200 205 210 215 220.

6 Feb 2019: LCSR only LCSR Lattice. 0 5 10 15 200. 1. 2. ... 3. 4. 5. q2. AV. ,0. 0 5 10 15 200.

22 Jan 2019: c) Evolution of the gap width for varying λ/d0. Results areshown for λ/d0 =0, 1, 5, 10, 20, 50, 100, 200, 500, 1000 and , and the three thickerlines correspond ... 0. -50. -100. -150. -200. 100. 10-1. 10-2¡. 10-310-4. 0. 100.

27 May 2019: This shortens the exposure timefrom 2 ms to 200–500 ms and allows us to obtain sharper imageswhile recording at high speed (300 fps).

6 Feb 2019: 200). The Laguerre polynomials obey therecurrence relation. (n 1)L(α)n1(ξ) = (2n 1 α ξ)L(α)n (ξ) (n α)L. (

22 Jul 2019: 2015); Tarduno et al. (2012)Eutectic composition Ce 32 wt% Ehlers (1972)Surface temperature Ts 200 KCoefficient of thermal expansivity $ 104 K1 Nimmo (2009)Activation energy E% 3 105 ... Recent paleomagnetic measurements found that theIVA iron meteorites

19 Jul 2019: 8. Atoms in Electromagnetic Fields. Our goal in this chapter is to understand how atoms interact with electromagnetic. fields. There will be several stages to our understanding. We start by looking at atoms. in constant, background electromagnetic

23 Jan 2019: bottom a herringbone texture with opening angle 2α = 90 made of chan-nels with width w = 1 mm separated by thin walls with thickness λ = 200 μm and height h [150,

27 Apr 2019: time. (s). 180. 50. 100. 150. 200. 250. 300. 350 UT1UT2Sep VarSpec. ... 40. 60. 80. 100. 120. 140. 160. 180. 200(a) (b). Figure 4.

19 Jul 2019: First some. – 200 –. notation. We describe the configuration of electrons by listing the hydrogen orbitals.

26 Nov 2019: Nonlinear systems for unconventional computing. Kirill P. Kalinin and Natalia G. Berloff. Abstract The search for new computational machines beyond the traditional vonNeumann architecture has given rise to a modern area of nonlinear science –

6 May 2019: order of Q ' 200–710 m3 s1.Hence, given the range of b0, the dimensionless flux could lie anywhere betweenQ̃ ' 2 109–6.5 103. ... till. These sizes varied significantly depending on the parameters,but for a typical simulation we used a domain 0 < r <

4 Nov 2019: A Life in Mathematical Science. Part I: Growing-Up, Student and Postdoc Years. Nicholas Stephen Manton FRS. Department of Applied Mathematics and Theoretical Physics,. University of Cambridge,. Wilberforce Road, Cambridge CB3 0WA, England. March

18 Oct 2019: a = 7 b=200. (See Mathematica: Blowflies, and keep b a).

8 Dec 2019: J. Fluid Mech. (2020), vol. 883, A18. c Cambridge University Press 2019doi:10.1017/jfm.2019.857. 883 A18-1. A theory for the slip and drag ofsuperhydrophobic surfaces with surfactant. Julien R. Landel1, François J. Peaudecerf2,‡, Fernando Temprano

25 Mar 2019: C H R I S T O P H E R E. T H O M A S. T H E S TA N D A R D M O D E L. L E N T T E R M 2 0 1 9. These notes are for use with the Part III lecture course The Standard Model, given in the Departmentof Applied Mathematics and Theoretical Physics,

16 Jul 2019: Let us reflect on the amplification of the measurement error. By our initial assumptionwe find that δ = ‖f fδ‖/‖A‖ ‖(0.01,0.01)>‖/2 =. 2/200. Moreover, the norm of. ... A†f =. 1/2 00 00 0. (f1f2. )=. f1/200. . Let

16 Jul 2019: By our initial assumption. we find that δ = ‖f fδ‖/‖K‖ ‖(0.01,0.01)>‖/2 =. 2/200. Moreover, the norm ofthe error in the reconstruction is then ‖uuδ‖ = ‖(20.01, ... K†f =. 1/2 00 00 0. (f1f2. )=. f1/200. .