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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.

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).

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.

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

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.

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,