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5 Apr 2016: 2), which gives. ψ cont0 (r) J0(kr) π. 2[γ ln(ka/2)] Y0(kr), (7). ... 9) of (kR)2/2π , and so describe the scattering correctto O((ka)4).

20 Jan 2016: 2mṙθ̇ mrθ̈ = ka sin(θ θB). d. dt. L. ṙ=L. ... r= mr̈ = mrθ̇2 kr ka cos(θ θB). d. dt. L.

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.

18 May 2016: Behavioral/Cognitive. Multimodal Feature Integration in the Angular Gyrus duringEpisodic and Semantic Retrieval. X Heidi M. Bonnici, Franziska R. Richter, Yasemin Yazar, and Jon S. SimonsDepartment of Psychology, University of Cambridge, Cambridge

22 Jul 2016: J Bacteriol. 1998; 180(9):2373–2378. PMID: 9573188. 35. Baldo L, Hotopp JCD, Jolley KA, Bordenstein SR, Biber SA, Choudhury RR, et al.

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: Representing the resonance between the modes @n,o,ka and by the label (n, k,, k,,), the solid circles represent (n, 1,l) resonances; the solid squares (n, 2,2) resonances;

12 Aug 2016: G?Gh3j|kA:?lH7aPG IP q 2! 6! > ,I, G G)?%c e %3:S&&$J0 )' ,-/./0 %3$H&( )4 5/./0 %dlH&=<>) )@ /B/.2?87%URF&=<>) )@ u/./ &2)5 )! ) ;!V @v _!

1 Oct 2016: J Phys Chem. (1927) 31:1663–8. doi: 10.1021/j150281a004. 32. Adapa S, Dingeldein H, Schmidt KA, Herald TJ.

4 Mar 2016: Small acoustically forced symmetric bodies in viscous fluids. François NadalCommissariat a l’Energie Atomique, 33114 Le Barp, France. Eric Laugaa). Department of Applied Mathematics and Theoretical Physics, University of Cambridge, Cambridge CB3