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27 Sep 2011: Insights into the Evolution of Vitamin B12 Auxotrophy fromSequenced Algal Genomes. Katherine E. Helliwell,1 Glen L. Wheeler,2,3 Kyriacos C. Leptos,4 Raymond E. Goldstein,4 andAlison G. Smith,1. 1Department of Plant Sciences, University of Cambridge,

30 Jul 2014: 8:23–29. doi: 10.1007/BF02353701.Brumley DR, Polin M, Pedley TJ, Goldstein RE. 2012.

21 Feb 2022: Day et al. eLife 2022;11:e72707. DOI: https:// doi. org/ 10. 7554/ eLife. 72707 1 of 28. Cellular organization in lab- evolved and extant multicellular species obeys a maximum entropy lawThomas C Day1, Stephanie S Höhn2, Seyed A Zamani- Dahaj1,3,4

18 May 2016: Coordinated beating of algal flagella is mediated bybasal couplingKirsty Y. Wana and Raymond E. Goldsteina,1. aDepartment of Applied Mathematics and Theoretical Physics, University of Cambridge, Cambridge CB3 0WA, United Kingdom. Edited by Peter Lenz

23 Sep 2015: elifesciences.org. RESEARCH ARTICLE. Cortical microtubule nucleation canorganise the cytoskeleton of Drosophilaoocytes to define the anteroposterior axisPhilipp Khuc Trong1,2, Hélène Doerflinger3, Jörn Dunkel1,4, Daniel St Johnston3,Raymond E

10 Apr 2011: R E S E A R C H A R T I C L E. Fluid dynamics of self-propelled microorganisms,from individuals to concentrated populations. Luis H. Cisneros Æ Ricardo Cortez ÆChristopher Dombrowski Æ Raymond E. Goldstein ÆJohn O. Kessler. Received: 13 February

2 Dec 2021: i. {avgj. ([Re(tj) RΞi (gtj)]. 2)}. i. , (S2). where i iterates over all datasets and j over all pointswithin the experimental dataset Re(tj) = Re(tj)/Re(0)enumerated by ... avgj. ([Re(tj) RΞ (gntj)]2. ). (S3). Here, all minimizations were performed

10 Apr 2011: J. Phys. II France 6 (1996) 767-796 MAY 1996, PAGE 767. Front Propagation in the Pearling Instability of Tubular Vesicles. Raymond E. Goldstein (), Philip Nelson (), Thomas Powers (>)and Udo Seifert (). () Joseph Henry Laboratory of Physics,

25 Sep 2015: FL47CH15-Goldstein ARI 1 December 2014 20:34. Green Algae as ModelOrganisms for BiologicalFluid DynamicsRaymond E. GoldsteinDepartment of Applied Mathematics and Theoretical Physics, Centre for MathematicalSciences, University of Cambridge,

10 Apr 2011: tJ.Se(T,Hcrit ) = Se(T,H--Hcrit ) - Se(T,H--Hcrit -). (17). where.tJ.Ms is the order parameter jump of the SM. ... tJ.Me(T ,Hcrit) = Me(T ,H--Hcrit ) - Me(T ,H--Hcrit -). (18).