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4 Jan 2011: 0.4. -15 -10 -5 0 5 10 15. f(λ 1. ,200. ). ... 0.4. -15 -10 -5 0 5 10 15. f(λ 2. ,200. ).

4 Jan 2011: For both initial conformations, we haveperformed 200 BH runs with 3000 steps each, resulting in atotal of 12 000 000 BH steps. ... Hence, we only allowed rotation around the z-axisand translation in the xy-plane for the generation of oligomers.The

4 Jan 2011: bodies: |Iy Iz| 200 and Ix/Iz 0.8.

13 Jan 2011: To as-sess accuracy, particularly at high densities, we carried outfour integrations for each crystal structure, at values of 2 / kBT equal to 50, 100, 150, and 200, where is ... 4.046 4.050F-FCC 200 5.000 24.15 1.531 1.602 H-F 270 3.704 767.4 4.579

13 Jan 2011: 25. 50. 75. 100. 0 50 100 150 200. G(n. ) / k.

13 Jan 2011: Following initial optimisation studies, in all subsequent calcu-lations (described later) the population size (which is constantwithin each GA run) was fixed at 200. ... d NuniqueNpop. ; ð6Þ. where Nunique is the number of unique (distinct) struc-tures

13 Jan 2011: The overall path complexity C P for roots1, 2, 3, and 4 of the BLN model is 0.215, 0.234, 0.200 and 0.135,respectively, but for root 1

13 Jan 2011: The GA parameter set is as fol-lows: population size = 200, maximum number ofgenerations = 200, crossover types = 1pt and 2pt, crossoverrate = 1.0, mutation rate = 0.1, elitism = 0.3, Monte

14 Jan 2011: Each simulation contains 120 A and 200 Bparticles, so that a maximum of ten target clusters could be formed. ... Eachsimulation contains 120 A, 200 B and 300 C particles, so that a maximum of ten target clusters could be formed.

14 Jan 2011: Controlling crystallization and its absence: proteins, colloids andpatchy modelsw. Jonathan P. K. Doye,a Ard A. Louis,b I-Chun Lin,c Lucy R. Allen,d. Eva G. Noya,e Alex W. Wilber,a Hoong Chwan Koke and Rosie Lyuse. Received 16th October 2006,