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14 Jan 2011: The stability of a crystal with diamond structure for patchy particleswith tetrahedral symmetry. Eva G. Noya,1,a Carlos Vega,2 Jonathan P. K. Doye,3 and Ard A. Louis41Instituto de Química Física Rocasolano, Consejo Superior de Investigaciones

13 Jul 2011: Thedifference in initial pressures between the smallest and thebiggest values of we have considered, = 1 and 105 s, isaround 0.24 atm with a difference in total excess work. ... J =dN. dt= bcNs. 0Nc , 24. where Nt is the number of nuclei formed in the

13 Jan 2011: bPV ln. QGmVT expðbAl0;n0Þ2. (24). Acknowledgements. This work was supported by the ERC (Advanced Grant agree-. ... 13 N. Geerts, T. Schmatko and E. Eiser, Langmuir, 2008, 24(9), 5118–5123.

4 Jan 2011: matrix can be replaced with similar matrices, such as correlation or sums-of-squares-cross-products (SSCP),24 depending on the application.

13 Jul 2011: W20. 09C. arlH. anse. rV. erla. g,M. unic. h,G. erm. any. ww. w.ij. mr. deN. otfo. rus. ein. inte. rnet. orin. tran. etsi. tes. Not. for. elec. tron. icdi. strib. utio. n. J. C. Schön, M. JansenMax-Planck-Institut für Festkörperforschung,

27 Jul 2011: Davis and Gray [24] first showed that in Hamiltonian systems with twodof, the transition state defined as the separatrix in the phase space is alwaysfree from barrier recrossings, so the transmission ... p. (p, q). cp2s1qt (2.24). q. (p, q). cp2sqt (2.25)

22 Jul 2011: 21, 22, 23, 24, 25, 26, 27, 28, 29, 30] for more information on structure prediction for the other.

27 Jul 2011: Chaotic dynamics in small inert gas clusters: The influence of potential energy saddles. Robert J. Hindea) and FL Stephen Berry D e p a r t m e n t of Chemistry a n d the J a m e s Franck Institute, T h e University of Chicago, 5 7 3 5 S o u t h