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10 Oct 2012: Ĥ = JN S2 B.Z.Xk! ka†kak O(S0) (2.16). where! k = 2JS(1 cos k) = 4JS sin2(k/2) represents the dispersion relation of the spinexcitations.

19 Jan 2012: detail, including a fluctuation-rounded stretch-coil transition of actin filaments. DOI: 10.1103/PhysRevLett.108.038103 PACS numbers: 87.16.Ka, 47.63.b, 83.50.Jf, 87.15.H.

10 May 2012: INTEGRABLE SYSTEMS. Maciej Dunajski. Department of Applied Mathematics and Theoretical Physics. University of Cambridge. Wilberforce Road, Cambridge CB3 0WA, UK. May 10, 2012. Contents. 1 Integrability in classical mechanics 41.1 Hamiltonian

1 Oct 2012: C A M B R I D G E U N I V E R S I T Y. REPORTERS p e c i a l N o 1 M o N d ay 1 o c t o b e r 2 0 1 2 Vol cxliii. p U b l i S H e d b y a U t H o r i t y. Deputy Vice-Chancellors appointed 2Chairmen of Syndicates, Boards, Committees, and other

17 Jan 2012: The microstructures of the weld nuggets are given inFig. 7 for cases where the current was 0?5 kA less thanImax. ... Table 4 Joint properties for commercial and investigated alloys. Carbon/wt-%Thickness/mm. Minimum weldcurrent/kA.

25 Nov 2012: Full lipid-binding curves used tocalculate Ka values are in Fig. S7. ... B) Protein–lipid FRET assays were per-formed with 5% PIP2 vesicles, and Ka was calculated for both 5 μM pY.

27 Nov 2012: So b′ = b ka is also in Λ and has. ... b′| = t′|a| < |a|. The choice of a tells us that b′ must be 0, so b = ka Za as required.

5 Jan 2012: 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

21 Mar 2012: ka. iii. JzJ. =. i. J. i. z. 1. i.

2 Nov 2012: Statutes and Ordinances of the University of Cambridge. Preceding: Chapter X. Following:CHAPTER XI. pp. 670–750. THE UNIVERSITY OFFICERS. Section 1. Section 2. Section 3. Revised edition 2012. The Chancellor, Masters and Scholars of the University