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3 Nov 2016: i. (-a-qOUa)Tii'-21 bl);' V,;(TJ;--l);)'}. (3) ora. ;. Here K0 and 11 are the nonsingular parts of the bulk and shear moduli. ... As a result, we write H in the form. (35). where = quaa and 11 = q 2/(Ko %tJ.)N.

20 Oct 2016: For correspondence: jss30@cam. ac.uk. †These authors contributed. equally to this work. Competing interests: The. authors declare that no. competing interests exist. Funding: See page 15. Received: 28 May 2016. Accepted: 26 September 2016.

22 Jul 2016: on July 22, 2016http://rspb.royalsocietypublishing.org/Downloaded from. rspb.royalsocietypublishing.org. ResearchCite this article: Martinez J, Cogni R, Cao C,Smith S, Illingworth CJR, Jiggins FM. 2016. Addicted? Reduced host resistance in.

24 Jan 2016: RESEARCH ARTICLE. A Polymorphism in the Processing BodyComponent Ge-1 Controls Resistance toa Naturally Occurring Rhabdovirus inDrosophilaChuan Cao, Michael M. Magwire¤a, Florian Bayer¤b, Francis M. Jiggins. Department of Genetics, University of

12 Aug 2016: P:?tJ. )3 ,0g 0! 0 aW TU ,! V ,=0 v L:s!

12 Aug 2016: J. Fluid Mech. (2013), vol. 722, pp. 554–595. c Cambridge University Press 2013 554doi:10.1017/jfm.2013.122. Invariant recurrent solutions embedded in aturbulent two-dimensional Kolmogorov flow. Gary J. Chandler and Rich R. Kerswell†. School of

23 Jul 2016: Dηn‖2 ‖ζn‖2 t‖ζn‖. t(1 t)rj=0. tj(1 ρ(A). )[ j2](‖ηn‖ ‖ζn‖ ‖ηn1‖ ‖ζn1‖). ... en1‖ ‖Den1‖2 ‖ωn1‖2 ‖en‖ t‖ωn‖. ‖Den‖2 ‖ωn‖2. t(1 t)rj=0. tj[‖f(j)t. (U(tn).

1 Oct 2016: 2002) 107:17–22. doi: 10.1016/S0169-328X(02)00441-2. 4. Dhaka A, Earley TJ, Watson J, Patapoutian A. ... J Phys Chem. (1927) 31:1663–8. doi: 10.1021/j150281a004. 32. Adapa S, Dingeldein H, Schmidt KA, Herald TJ.

25 Feb 2016: FL48CH05-Lauga ARI 24 November 2015 12:50. Bacterial HydrodynamicsEric LaugaDepartment of Applied Mathematics and Theoretical Physics, Center for MathematicalSciences, University of Cambridge, Cambridge CB3 0WA, United Kingdom;email:

2 Jun 2016: 23. where we definet̃i = εij tj , ̃i = εijj , (7.3).