Search

10 Jun 2014: of UTC. – The end-point (server, S) in domain with name D has KA and a clock withint′ of UTC. – ... onp. 8). [24] Colin Percival. Stronger key derivation via sequential memory-hard functions.05/2009.

30 Jun 2014: a n d L e i l a M a l i ka for p roof re a d i ng a n d. ... d-p a r t y " , r equ i r i ng-e x p l ic i t -conse n t " , a n d u n l i n ka

26 Nov 2014: m(i)k1|k = Akm. (i)k|k (22). P(i)k1|k = AkP. (i)k|kA. Tk Qk. ... j)k|kA. Tk ,. ν(i)k1|k = λνν. (j)k|k, Ψ. (i)k1|k = λΨΨ.

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

7 Oct 2014: tred around the concept of symmetry reduction. It was noted by Richard Ward [24].

26 Jun 2014: teins, including α-synuclein (23, 24), can grow most efficientlyby the addition of oligomers to the fibril ends. ... Conway KA, Harper JD, Lansbury PT (1998) Accelerated in vitro fibril formation by a mu-.