-
15
-
-
7244261407
-
-
G. O. Sitz, A. C. Kummel, R. N. Zare, and J. C. Tully, J. Chem. Phys. 89, 2572 (1988).
-
(1988)
J. Chem. Phys.
, vol.89
, pp. 2572
-
-
Sitz, G.O.1
Kummel, A.C.2
Zare, R.N.3
Tully, J.C.4
-
16
-
-
0000050919
-
-
C. R. Arumainayagam, R. J. Madix, M. C. McMaster, V. M. Suzawa, and J. C. Tully, Surf. Sci. 226, 180 (1990).
-
(1990)
Surf. Sci.
, vol.226
, pp. 180
-
-
Arumainayagam, C.R.1
Madix, R.J.2
McMaster, M.C.3
Suzawa, V.M.4
Tully, J.C.5
-
17
-
-
0342641009
-
-
M. Head-Gordon, J. C. Tully, C. T. Rettner, B. Mullins, and D. J. Auerbach, J. Chem. Phys. 94, 1516 (1991).
-
(1991)
J. Chem. Phys.
, vol.94
, pp. 1516
-
-
Head-Gordon, M.1
Tully, J.C.2
Rettner, C.T.3
Mullins, B.4
Auerbach, D.J.5
-
30
-
-
0001286606
-
-
M. Head-Gordon, J. C. Tully, H. Schlichting, and D. Menzel, J. Chem. Phys. 95, 9266 (1991).
-
(1991)
J. Chem. Phys.
, vol.95
, pp. 9266
-
-
Head-Gordon, M.1
Tully, J.C.2
Schlichting, H.3
Menzel, D.4
-
32
-
-
0001324268
-
-
C. R. Arumainayagam, M. C. McMaster, G. R. Schoofs, and R. J. Madix, Surf. Sci. 222, 213 (1989).
-
(1989)
Surf. Sci.
, vol.222
, pp. 213
-
-
Arumainayagam, C.R.1
McMaster, M.C.2
Schoofs, G.R.3
Madix, R.J.4
-
35
-
-
0001104458
-
-
C. R. Arumainayagam, G. R. Schoofs, M. C. McMaster, and R. J. Madix, J. Phys. Chem. 95, 1041 (1991).
-
(1991)
J. Phys. Chem.
, vol.95
, pp. 1041
-
-
Arumainayagam, C.R.1
Schoofs, G.R.2
McMaster, M.C.3
Madix, R.J.4
-
40
-
-
85033848062
-
-
note
-
i and is sometimes referred to as "negative"energy scaling.
-
-
-
-
42
-
-
0002561060
-
-
edited by D. Langreth and H. Suhl Academic, New York
-
J. C. Tully, in Many Body Phenomena at Surfaces, edited by D. Langreth and H. Suhl (Academic, New York, 1984), p. 377.
-
(1984)
Many Body Phenomena at Surfaces
, pp. 377
-
-
Tully, J.C.1
-
44
-
-
85033847235
-
-
Sowa et al. used LEED intensity-voltage spectra to determine that interlayer spacing for the first four layers contract, with the first layer contracting the most and the subsequent layers contracting less with increasing depth. They also determined that platinum atoms in the second and fourth layers move toward the missing row, producing a slightly buckled trough
-
Sowa et al. used LEED intensity-voltage spectra to determine that interlayer spacing for the first four layers contract, with the first layer contracting the most and the subsequent layers contracting less with increasing depth. They also determined that platinum atoms in the second and fourth layers move toward the missing row, producing a slightly buckled trough.
-
-
-
-
53
-
-
0004161642
-
-
Wiley, New York
-
R. N. Zare, Angular Momentum (Wiley, New York, 1987), pp. 77-81.
-
(1987)
Angular Momentum
, pp. 77-81
-
-
Zare, R.N.1
-
54
-
-
85033868653
-
-
note
-
The measured energies of adsorption from temperature programmed desorption for ethane and propane on Pt(111) are 32±4 kJ/mol (Ref. 35) and 44±2 kJ/mol (Ref. 37). respectively. This value for methane on Pt(111) has not been determined. The stochastic trajectory simulations employing the single methyl-platinum potential assigns a total energy of adsorption for methane, ethane, and propane on Pt(111) of 14, 28, and 44 kJ/mol. respectively, in good agreement with the experimental values for ethane and propane on this surface. Using these energies as cutoffs and comparing the initial trapping probabilities from experiment and theory of each alkane on Pt(111) at each cutoff energy shows trapping is at least greater than 0.2 for all of the alkanes, with propane followed by ethane displaying the largest trapping at the cutoff energies.
-
-
-
-
55
-
-
85033853880
-
-
note
-
Temperature programmed desorption of methane from Pt(111) beginning at a surface temperature of 95 K exhibited a single peak at 140 K with a coverage of less than 0.01 ML (Ref. 32). The origin of this desorption was attributed to adsorption on defect sites of Pt(111). Consequently, the first layer adsorption state of methane from Pt(111) was thus believed to be less than 95 K.
-
-
-
-
56
-
-
0006969785
-
-
D. P. Masson, T. F. Hanisco, W. L. Nichols, C. Yan, A. C. Kummel, and J. C. Tully, J. Chem. Phys. 101, 3341 (1994).
-
(1994)
J. Chem. Phys.
, vol.101
, pp. 3341
-
-
Masson, D.P.1
Hanisco, T.F.2
Nichols, W.L.3
Yan, C.4
Kummel, A.C.5
Tully, J.C.6
-
57
-
-
85033834199
-
-
unpublished experimental data
-
57M. C. McMaster (unpublished experimental data).
-
-
-
McMaster, M.C.1
-
58
-
-
85033843127
-
-
note
-
Classical turning point away from the surface is strictly defined as the point where the z-direction center of mass velocity of the molecule changes sign from positive to negative. The negative direction is into the surface.
-
-
-
-
59
-
-
85033833469
-
-
note
-
Because of previous simulations of ethane on Pt(111) (Ref. 19) and Pt(110)-(1×2) (Ref. 20) which divided rotational excitation into two motions, cartwheel and helicopter, and in order examine the energy transfer mechanisms for propane on these surfaces, the notions of cartwheel and helicopter rotational motions were retained for propane. Analogous to helicopter rotational motion for ethane, the magnitude of rotational energy for propane with the angular momentum vector (J) directed along the surface normal (z direction) was designated as helicopter rotational energy. Cartwheel rotational energy for propane was calculated by determining the total rotational energy of the molecule and subtracting the amount helicopter rotational energy. This definition is also consistent with the notion of cartwheel motion for ethane since the cartwheel designation for propane has its J vector parallel to the surface (x-y plane).
-
-
-
-
60
-
-
85033840373
-
-
note
-
This method of analysis was used previously to determine the relative roles of the energy storage mechanisms available to assist ethane trapping on Pt(111) (Ref. 19) and Pt(110)-(1×2) (Ref. 20).
-
-
-
-
64
-
-
85033860197
-
-
note
-
This information for methane on Pt(111) was not presented in Table V because α at this angle (60°) is considerably lower than the initial trapping probabilities of ethane and propane on Pt(111) and thus cannot be appropriately compared.
-
-
-
-
66
-
-
21844505250
-
-
J. L. W. Siders and G. O. Sitz, J. Chem. Phys. 101, 6264 (1994); J. Vac. Sci. Tech. A 13, 1400 (1995).
-
(1995)
J. Vac. Sci. Tech. A
, vol.13
, pp. 1400
-
-
-
67
-
-
0001347027
-
-
C. T. Rettner, J. Kimman, F. Fahre, D. J. Auerbach, and H. Morawitz, Surf. Sci. 192, 107 (1987).
-
(1987)
Surf. Sci.
, vol.192
, pp. 107
-
-
Rettner, C.T.1
Kimman, J.2
Fahre, F.3
Auerbach, D.J.4
Morawitz, H.5
-
68
-
-
3543084755
-
-
C. T. Rettner, F. Fabre, J. Kimman, and D. J. Auerbach, Phys. Rev. Lett. 55, 1904 (1985).
-
(1985)
Phys. Rev. Lett.
, vol.55
, pp. 1904
-
-
Rettner, C.T.1
Fabre, F.2
Kimman, J.3
Auerbach, D.J.4
-
70
-
-
85033867290
-
-
note
-
The degree of shadowing on Pt(110)-(1×2) suggested for propane, however, is slightly less than what was indicated for ethane. This comparison, however, might be complicated by two effects: First, the use of center of mass positions for propane, which is less appropriate at representing the precise position of impact for molecules with increasing complexity, might tend to blur shadowing effects and suggest less shadowing than actually felt. Second, it is not clear which incident energy of ethane and propane along the rough azimuth should be compared to each other.
-
-
-
|