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7 Jun 2011: You may view additional information on a particular element. Simply click on the element's name or formula in the table below. Pictures representing each element are avaiable on ChemSoc's Visual Elements site. 2. 13. 14. 15. 16. 17. 2. 3. 4. 5. 6.

6 Jan 2011: C(sp3) 65 11 14 4.6000 1.1130 1.1144 0.003 O1 0 H-C(sp3) 65 ANGLES, BEND AND STRETCH BEND ENERGIES 24 Bend interactions present -------------------------------------- Atom Numbers

6 Jan 2011: Formula. Energy. Structure. Formula. Energy. Structure. C. 11. H. 24. 28.11. ... 16. 17.24. C. 3. H. 8. 6.27. C. 8. H. 18.

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

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)

4 Jan 2011: S. Berry, J. Phys. B 24, L351 1991. 10 B. Eckhardt and D. ... Many-Particle Lyapunov Vectors 2004 http://arxiv.org/abs/nlin/0404028. 24 H. Abarbanel, R. Brown, and M.

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.

4 Jan 2011: Address correspondence todw34@cam.ac.uk. Received for review October 4, 2009and accepted December 24, 2009. ... 24. Wales, D. J. Discrete Path Sampling. Mol. Phys. 2002, 100,3285–3306.

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

4 Jan 2011: aðq jÞ@q j;g. q j0. 1. 2pn j;g. 24. 35. 2. ... Annu Rev PhysChem 1997, 48:545-600. 24. Miller MA, Wales DJ: Energy landscape of a model protein.J Chem Phys 1999, 111:6610-6616.