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14 Jul 2014: 22–24), corresponding to the case of flagella behind orin front of the cell body. ... J Phys Condens Matter 24(6):065101. 38. Peskin CS (2002) The immersed boundary method.

7 Oct 2014: Proc Natl Acad SciUSA 96(26):14854–14859. 18. Scott KA, Randles LG, Clarke J (2004) The folding of spectrin domains II: Phi-valueanalysis of R16. ... Nat Struct Biol 9(3):209–216. 35. Ozkan SB, Bahar I, Dill KA (2001) Transition states and the

1 Oct 2014: Statutes and Ordinances of the University of Cambridge. A LevelsChap. II 3. Abbott Fund and ExhibitionsAbbott, C.C., FundChap. XII 2. Abrahamic Faiths and Shared Values, Sultan Qaboos ProfessorChap. XI 3. Academic staffappealsSche. - Academic Staff 5

19 Feb 2014: Statutes and Ordinances of the University of Cambridge. Please note, index references to items contained in Statute currently link to the 2013 Statutes, which have since been repealed. Please refer to the new Statutes and Special Ordinances,

25 Nov 2014: Recent research hasshown that even after significant cycling stressing, the austenite films ofnanostructured bainite in the regions of maximum subsurface shear stressdo not stress transform to martensite [24]. ... 24] W. Solano-Alvarez, E. J. Pickering, H

18 Jan 2014: 21. Prabhu NV, Sharp Ka (2005) Heat capacity in proteins. Annu Rev Phys Chem. ... 2001) Sequence. complexity of disordered protein. Proteins 42: 38–48.24. Deechongkit S, Nguyen H, Powers ET, Dawson PE, Gruebele M, et al.

30 Jul 2014: Funding: See page 14. Received: 11 March 2014Accepted: 24 June 2014Published: 29 July 2014.

10 Nov 2014: ARTICLE. Received 24 Jan 2014 | Accepted 19 Sep 2014 | Published 10 Nov 2014. ... It comes from TO phononsaround the Brillouin Zone (BZ) edge K16,22, is active by doubleresonance (DR)24, and is strongly dispersive with excitationenergy due to a Kohn

24 Apr 2014: and is characterized by four non-dimensional numbers:. Pe= kBTAλ2a. ηf D2, Da= Ka. ... c̃1ρ+ c̃1 φ̃0. ρ=(c c̃0)φ̃1. ρk(ζ)Da k(ζ)c̃0. (3.24). Phoretic self-propulsion at finite Péclet numbers 581.

6 Oct 2014: components, the possible holonomy groups of these irreducible non–symmetric. Riemannian manifolds have been classified by Berger [24]. ... τ := ξA′(dξA. ′ ξB. ′ΓA. ′B′. ). (2.24). Using τ, we can lift the vector fields ξA′AA′ to F