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

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: 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?

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.

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

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. (

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 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.

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: 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.