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7 Jun 2010: 35T;w38s35/2NQRD2/2A.8;-0:K/l$N2O8HN2-7=;?%603nLK+@=X<h+.=>QR:K=>aOTX360-7/2n3G={A@:Ka]42-0/F3t8H-0:5/q:5Q&n35AsN$N2-0?2?P+@/vD2/ ... J8HGl -7IK+./d8HNF3G88;N2+<@=;T>:K/9?2=H3niST8H-0a9+@TyR=;.<26z35A.-0/21_8;N2+4F356760T#:5/O+@35AsNO:fA@A@35T;-7:K/»QR=>

7 Jun 2010: The specific values of kA and n depend on the natureof nucleation and growth. ... p. 216. Table 3 Values of ln kA for each crystallisationtemperature from normalised data.

7 Jun 2010: Substituting for ψ(x) we get: A sin kaB cos ka = 0 (1). ... A sin kaB cos ka = 0 (3). Adding equations (1) and (3) gives: 2Bcos(ka) = 0.

12 May 2010: Institute/Li Ka Shing Centre; Faculty of Education; Institute of Criminology;Department of Chemistry (Photo: Nathan Pitt); Institute for Manufacturing; Kavli Institute forCosmology at Cambridge; Wellcome Trust and Cancer Research UK

4 Apr 2010: The first indication of unusual behaviour in the two-dimensional XY -model (n = 2)appeared in an analysis of the high temperature series expansion by Stanley and Ka-plan (1971).

7 Jun 2010: force of 1.69 kN and a peak current of 8.1 kA. ... a) (b). (c) (d). Figure 3: Resistance spot weld produced using interstitial–free steel with 7 kA current, 30 cyclesweld time [3] (reproduced with permission of B.

8 Apr 2010: 210). for some one–form Ka. Note that (210) follows from (28) withK A A′ = ω B′A′ ϒB′ A, (211). ... Then (29, 210, 215) must hold with. constant , in which case Ka vanishes but from (215) we deduce = 0 ; φA B A′ B′ = ωA′ B′ ρA B.

29 Oct 2010: It is housed in the Li Ka Shing Centre, a state-of-the-art research facility located on the Cambridge Biomedical Campus which was generously funded by Hutchison Whampoa Ltd, Cambridge

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4 Jan 2010: The advent of new technologies has enabled researchers to interrogate human genomes at unprecedented resolution. These technologies have led to a wealth of