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The disadvantage of these types of clusters arises from the difficulty in the synthesis process and scaling. The systems of graphene nanoribbons Fig. 13. Time taken by the signal to travel from one end to the other of the automaton as a function of the total number of cells The simulation was performed for J = 150 meV and T = 300 K. Different curves represent simulations with distinct number of control cells. 32 Cellular Automata - Innovative Modelling for Science and Engineering proposed in this work are scalable for working at room temperature.

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Microelectron. J. 39, 1239. ; Shen, P. & Chen, Z. (2009). J. Phys. Chem C 113, 15043. Lu, Y. H. & Feng, Y. P. (2009). J. Phys. Chem C 113, 20841. Macucci, M. (2006). Quantum Cellular Automata, Imperial College Press, ISBN 1-86094-632-1, London, United Kingdom. Nielsen, M. A. & Chuang, I. L. (2003). Quantum Computation and Quantum Information, Cambridge University Press, ISBN 0-521-63503-9, Cambridge, United Kingdom. ; Dresselhaus, G. & Dresselhaus M. S. (1996). Phys. Rev. B 54, 17954. Nonoselov, K.

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