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4
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0000305993
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S. Andersson, L. Wilzén, M. Persson, and J. Harris, Phys. Rev. B 40, 8146 (1989).
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Andersson, S.1
Wilzén, L.2
Persson, M.3
Harris, J.4
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5
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0343311238
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note
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2 is desorbed by the laser pulses a low rale of dissociation is observed presumably due to an electronic excitation mechanism.
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8
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5044235354
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i = 0 where θ, is the scattering angle: see R. G. Rowe, L. Rathbun, and G. Ehrlich, Phys. Rev. Lett. 35, 1104 (1975).
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Phys. Rev. Lett.
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Rowe, R.G.1
Rathbun, L.2
Ehrlich, G.3
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12
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0342876193
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Rarefied Gas Dynamics, edited by R. Camparque (Commisarat a l'Energie Atomique, Paris)
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K. Winkelmann, in Rarefied Gas Dynamics, Proceedings of the 11th International Symposium Vol. II, edited by R. Camparque (Commisarat a l'Energie Atomique, Paris, 1979).
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Proceedings of the 11th International Symposium
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Winkelmann, K.1
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13
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6144230113
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F. Althoff, T. Andersson, and S. Andersson, Phys. Rev. Lett, 79, 4429 (1997).
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Phys. Rev. Lett
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Althoff, F.1
Andersson, T.2
Andersson, S.3
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14
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4243727696
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J. Kimman, C. T. Rettner, D. J. Auerbach, J. A. Barker, and J. C. Tully, Phys. Rev. Lett. 57, 2053 (1986).
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Phys. Rev. Lett.
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Kimman, J.1
Rettner, C.T.2
Auerbach, D.J.3
Barker, J.A.4
Tully, J.C.5
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17
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24644457620
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J. Harris and P. J. Feibelman, Surf. Sci. 115, L133 (1982); J. O. Hirschfelder, C. F. Curtiss, and R. B. Bird, Molecular Theory of Gases and Liquids (Wiley, New York, 1954).
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Surf. Sci.
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Harris, J.1
Feibelman, P.J.2
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18
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0003556247
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Wiley, New York
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J. Harris and P. J. Feibelman, Surf. Sci. 115, L133 (1982); J. O. Hirschfelder, C. F. Curtiss, and R. B. Bird, Molecular Theory of Gases and Liquids (Wiley, New York, 1954).
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(1954)
Molecular Theory of Gases and Liquids
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Hirschfelder, J.O.1
Curtiss, C.F.2
Bird, R.B.3
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19
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0342876189
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note
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R was chosen so that V(z,θ) reproduces, at the classical turning point of the molecule, the anisotropy of a potential that was determined from total energy calculations, involving a lateral average over the top, bridge, and hollow sites. The calculations were performed with the plane-wave pseudopotential code DACAPO [DACAPO-1.30 of B. Hammer et al., CAMP, DTH, Lyngby, Denmark], using the generalized gradient approximation for the exchange-correlation energy. The calculational unit cell contained a slab of four layers of Cu ions with three ions in each layer, resulting in a 4.47 Å separation between the molecules. The Cu slabs were separated by a vacuum layer that was five layers thick. The ion cores were represented by ultrasoft pseudopotentials, enabling a plane wave expansion cutoff at 30 Ry, and the surface Brillouin zone was sampled by 54 k points.
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20
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0001051562
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L. Wilzén, F. Althoff, S. Andersson, and M. Persson, Phys. Rev. B 43, 7003 (1991).
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Phys. Rev. B
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Wilzén, L.1
Althoff, F.2
Andersson, S.3
Persson, M.4
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23
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0342876187
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note
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In an extension of the work presented here, we plan to incorporate the effect of phonon losses in the calculations via a phenomenological optical potential.
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