-
1
-
-
0001242544
-
-
references contained therein
-
L. W. Bruch, A. P. Graham, and J. P. Toennies, J. Chem. Phys. 112, 3314 (2000), and references contained therein.
-
(2000)
J. Chem. Phys.
, vol.112
, pp. 3314
-
-
Bruch, L.W.1
Graham, A.P.2
Toennies, J.P.3
-
3
-
-
0036644120
-
-
F. Brunet, R. Schaub, S. Féderigo, R. Monot, J. Buttet, and W. Harbich, Surf. Sci. 512, 201 (2002).
-
(2002)
Surf. Sci.
, vol.512
, pp. 201
-
-
Brunet, F.1
Schaub, R.2
Féderigo, S.3
Monot, R.4
Buttet, J.5
Harbich, W.6
-
4
-
-
84979718473
-
-
B. Grimm, H. Hövel, M. Pollmann, and B. Reihl, Phys. Rev. Lett. 83, 991 (1999);
-
(1999)
Phys. Rev. Lett.
, vol.83
, pp. 991
-
-
Grimm, B.1
Hövel, H.2
Pollmann, M.3
Reihl, B.4
-
5
-
-
85039030670
-
-
(private communication)
-
H. Hövel (private communication).
-
-
-
Hövel, H.1
-
6
-
-
0035883665
-
-
G. Benedek, G. Brusdeylins, V. Senz, J. G. Skofronick, J. P. Toennies, F. Traeger, and R. Vollmer, Phys. Rev. B 64, 125421 (2001);
-
(2001)
Phys. Rev. B
, vol.64
, pp. 125421
-
-
Benedek, G.1
Brusdeylins, G.2
Senz, V.3
Skofronick, J.G.4
Toennies, J.P.5
Traeger, F.6
Vollmer, R.7
-
7
-
-
85039025998
-
-
2/MgO(001). This included the Beeby correction for an attractive well of depth 3 meV and an angle-factor following
-
2/MgO(001). This included the Beeby correction for an attractive well of depth 3 meV and an angle-factor following
-
-
-
Traeger, F.1
-
8
-
-
0000032491
-
-
h than on its attractive well. For some cautionary remarks on use of the eikonal analysis to estimate the topography of strongly corrugated systems
-
h than on its attractive well. For some cautionary remarks on use of the eikonal analysis to estimate the topography of strongly corrugated systems, see
-
(1975)
Surf. Sci.
, vol.48
, pp. 649
-
-
Garribaldi, U.1
Levi, A.C.2
Spadacini, R.3
Tommei, G.4
-
14
-
-
0000222343
-
-
P. Zeppenfeld, U. Becher, K. Kern, and G. Comsa, J. Electron Spectrosc. Relat. Phenom. 54, 265 (1990).
-
(1990)
J. Electron Spectrosc. Relat. Phenom.
, vol.54
, pp. 265
-
-
Zeppenfeld, P.1
Becher, U.2
Kern, K.3
Comsa, G.4
-
15
-
-
33744821712
-
-
H. Taub, K. Carneiro, J. K. Kjems, L. Passell, and J. P. McTague, Phys. Rev. B 16, 4551 (1977).
-
(1977)
Phys. Rev. B
, vol.16
, pp. 4551
-
-
Taub, H.1
Carneiro, K.2
Kjems, J.K.3
Passell, L.4
McTague, J.P.5
-
17
-
-
0037438290
-
-
J. G. Skofronick, J. P. Toennies, F. Traeger, and H. Weiss, Phys. Rev. B 67, 035413 (2003).
-
(2003)
Phys. Rev. B
, vol.67
, pp. 035413
-
-
Skofronick, J.G.1
Toennies, J.P.2
Traeger, F.3
Weiss, H.4
-
21
-
-
85039028932
-
-
The isotropic models used in the present work are chosen because they have been used in modeling of the monolayer solids and because it seems more consistent to include estimates of the effect of the substrate anisotropy on both the attractive and repulsive terms of the potential. This procedure has been discussed previously for the series He, Ne, and Kr on graphite:
-
The isotropic models used in the present work are chosen because they have been used in modeling of the monolayer solids and because it seems more consistent to include estimates of the effect of the substrate anisotropy on both the attractive and repulsive terms of the potential. This procedure has been discussed previously for the series He, Ne, and Kr on graphite:
-
-
-
-
22
-
-
0003864917
-
-
H. Taub, G. Torzo, H. J. Lauter, and S. C. Fain, Jr. (Plenum, New York
-
L. W. Bruch, in Phase Transitions in Surface Films II, edited by H. Taub, G. Torzo, H. J. Lauter, and S. C. Fain, Jr. (Plenum, New York, 1991), p. 67.
-
(1991)
Phase Transitions in Surface Films II
, pp. 67
-
-
Bruch, L.W.1
-
23
-
-
0000819359
-
-
G. Vidali, G. Ihm, H.-Y. Kim, and M. W. Cole, Surf. Sci. Rep. 12, 133 (1991).
-
(1991)
Surf. Sci. Rep.
, vol.12
, pp. 133
-
-
Vidali, G.1
Ihm, G.2
Kim, H.-Y.3
Cole, M.W.4
-
25
-
-
3342972338
-
-
J. Braun, D. Fuhrmann, A. S¨iber, B. Gumhalter, and Ch. Wöll, Phys. Rev. Lett. 80, 125 (1998).
-
(1998)
Phys. Rev. Lett.
, vol.80
, pp. 125
-
-
Braun, J.1
Fuhrmann, D.2
S¨Iber, A.3
Gumhalter, B.4
Wöll, C.5
-
26
-
-
0000418473
-
-
Ch. Ramseyer, V. Pouthier, C. Girardet, P. Zeppenfeld, M. Büchel, V. Diercks, and G. Comsa, Phys. Rev. B 55, 13 203 (1997).
-
(1997)
Phys. Rev. B
, vol.55
, pp. 13 203
-
-
Ramseyer, C.1
Pouthier, V.2
Girardet, C.3
Zeppenfeld, P.4
Büchel, M.5
Diercks, V.6
Comsa, G.7
-
28
-
-
0000471455
-
-
F. Y. Hansen, V. L. P. Frank, H. Taub, L. W. Bruch, H. J. Lauter, and J. R. Dennison, Phys. Rev. Lett. 64, 764 (1990).
-
(1990)
Phys. Rev. Lett.
, vol.64
, pp. 764
-
-
Hansen, F.Y.1
Frank, V.L.P.2
Taub, H.3
Bruch, L.W.4
Lauter, H.J.5
Dennison, J.R.6
-
30
-
-
0000986997
-
-
4He/graphite from band structure effects in selective adsorption resonance data
-
4He/graphite from band structure effects in selective adsorption resonance data [M. W. Cole, D. R. Frankl, and D. L. Goodstein, Rev. Mod. Phys. 53, 199 (1981)].
-
(1981)
Rev. Mod. Phys.
, vol.53
, pp. 199
-
-
Cole, M.W.1
Frankl, D.R.2
Goodstein, D.L.3
-
32
-
-
0000364841
-
-
references contained therein
-
Th. Seyller, M. Caragiu, R. D. Diehl, P. Kaukasoina, and M. Lindroos, Phys. Rev. B 60, 11 084 (1999), and references contained therein.
-
(1999)
Phys. Rev. B
, vol.60
, pp. 11 084
-
-
Seyller, T.1
Caragiu, M.2
Diehl, R.D.3
Kaukasoina, P.4
Lindroos, M.5
-
35
-
-
85039021372
-
-
Ph.D. thesis, University of Washington–Seattle
-
C. G. Shaw, Ph.D. thesis, University of Washington–Seattle, 1979.
-
(1979)
-
-
Shaw, C.G.1
-
36
-
-
0001473115
-
-
B. Hall, D. L. Mills, P. Zeppenfeld, K. Kern, U. Becher, and G. Comsa, Phys. Rev. B 40, 6326 (1989).
-
(1989)
Phys. Rev. B
, vol.40
, pp. 6326
-
-
Hall, B.1
Mills, D.L.2
Zeppenfeld, P.3
Kern, K.4
Becher, U.5
Comsa, G.6
-
37
-
-
0008823272
-
-
K. L. D’Amico, J. Bohr, D. E. Moncton, and D. Gibbs, Phys. Rev. B 41, 4368 (1990).
-
(1990)
Phys. Rev. B
, vol.41
, pp. 4368
-
-
D’Amico, K.L.1
Bohr, J.2
Moncton, D.E.3
Gibbs, D.4
-
38
-
-
85038973477
-
-
In this work, the substrate is treated as static. Although there is an adsorbate-substrate potential energy, there is no provision for the hybridization (Refs. 7 and 24) of adlayer and substrate dynamics that occurs close to the adlayer Brillouin zone center for some degrees of freedom
-
In this work, the substrate is treated as static. Although there is an adsorbate-substrate potential energy, there is no provision for the hybridization (Refs. 7 and 24) of adlayer and substrate dynamics that occurs close to the adlayer Brillouin zone center for some degrees of freedom.
-
-
-
-
43
-
-
33751226701
-
-
D. Degenhardt, H. J. Lauter, and R. Haensel, Jpn. J. Appl. Phys., Suppl. 26(3), 341 (1987).
-
(1987)
Jpn. J. Appl. Phys., Suppl.
, vol.26
, Issue.3
, pp. 341
-
-
Degenhardt, D.1
Lauter, H.J.2
Haensel, R.3
-
47
-
-
0039926452
-
-
A. Frigo, F. Toigo, M. W. Cole, and F. O. Goodman, Phys. Rev. B 33, 4184 (1986).
-
(1986)
Phys. Rev. B
, vol.33
, pp. 4184
-
-
Frigo, A.1
Toigo, F.2
Cole, M.W.3
Goodman, F.O.4
-
48
-
-
85039014432
-
-
2 molecules in the j = 1, m = ±1 state
-
2 molecules in the j = 1, m = ±1 state.
-
-
-
-
49
-
-
85038978428
-
-
2 in adsorption isotherms at about 18 K gives some evidence against this proposal
-
2 in adsorption isotherms at about 18 K gives some evidence against this proposal.
-
-
-
-
50
-
-
0004076366
-
-
A. F. G. Wyatt and H. J. Lauter (Plenum, New York
-
See O. E. Vilches, F. C. Liu, D. L. Kingsbury, J. Ma, M. Bienfait, J. Suzanne, J. M. Gay, M. Maruyama, P. Zeppenfeld, D. Degenhardt, H. J. Lauter, F. Rieutord, and G. Coddens, in Excitations in Two-Dimensional and Three-Dimensional Quantum Fluids, edited by A. F. G. Wyatt and H. J. Lauter (Plenum, New York, 1991), p. 477.
-
(1991)
Excitations in Two-Dimensional and Three-Dimensional Quantum Fluids
, pp. 477
-
-
Vilches, O.E.1
Liu, F.C.2
Kingsbury, D.L.3
Ma, J.4
Bienfait, M.5
Suzanne, J.6
Gay, J.M.7
Maruyama, M.8
Zeppenfeld, P.9
Degenhardt, D.10
Lauter, H.J.11
Rieutord, F.12
Coddens, G.13
-
51
-
-
0000259156
-
-
L. Mattera, F. Rosatelli, C. Salvo, F. Tommasini, U. Valbusa, and G. Vidali, Surf. Sci. 93, 515 (1980).
-
(1980)
Surf. Sci.
, vol.93
, pp. 515
-
-
Mattera, L.1
Rosatelli, F.2
Salvo, C.3
Tommasini, F.4
Valbusa, U.5
Vidali, G.6
-
52
-
-
85039027819
-
-
2〉/2) and the force constant for ω0, is a weighted average of the contributions from the a and b sites of the HOC unit cell. The assumed exponential dependence is consistent with the large difference for the corrugation amplitudes of Xe/Cu at two values of g in Table I
-
∥ is a weighted average of the contributions from the a and b sites of the HOC unit cell. The assumed exponential dependence is consistent with the large difference for the corrugation amplitudes of Xe/Cu at two values of g in Table I.
-
-
-
|