-
2
-
-
0030946437
-
-
A. C. Dillon, K. M. Jones, T. A. Bekkedahl, C. H. Kiang, D. S. Bethune, and M. J. Heben, Nature 386, 377 (1997); E. B. Mackie, R. A. Wolfson, L. M. Arnold, K. Lafdi and A. D. Migone, Langmuir 13, 7197 (1997).
-
(1997)
Nature
, vol.386
, pp. 377
-
-
Dillon, A.C.1
Jones, K.M.2
Bekkedahl, T.A.3
Kiang, C.H.4
Bethune, D.S.5
Heben, M.J.6
-
3
-
-
0031360210
-
-
A. C. Dillon, K. M. Jones, T. A. Bekkedahl, C. H. Kiang, D. S. Bethune, and M. J. Heben, Nature 386, 377 (1997); E. B. Mackie, R. A. Wolfson, L. M. Arnold, K. Lafdi and A. D. Migone, Langmuir 13, 7197 (1997).
-
(1997)
Langmuir
, vol.13
, pp. 7197
-
-
Mackie, E.B.1
Wolfson, R.A.2
Arnold, L.M.3
Lafdi, K.4
Migone, A.D.5
-
4
-
-
0031651628
-
-
G. Stan and M. W. Cole, Surf. Sci. 395, 280 (1998) and J. Low Temp. Phys. 110, 539 (1998); and private communications from M. Bienfait, J. K. Johnson, M. H. W. Chan, A. D. Migone and H. K. Kim.
-
(1998)
Surf. Sci.
, vol.395
, pp. 280
-
-
Stan, G.1
Cole, M.W.2
-
5
-
-
0031676695
-
-
G. Stan and M. W. Cole, Surf. Sci. 395, 280 (1998) and J. Low Temp. Phys. 110, 539 (1998); and private communications from M. Bienfait, J. K. Johnson, M. H. W. Chan, A. D. Migone and H. K. Kim.
-
(1998)
J. Low Temp. Phys.
, vol.110
, pp. 539
-
-
-
6
-
-
0031651628
-
-
private communications
-
G. Stan and M. W. Cole, Surf. Sci. 395, 280 (1998) and J. Low Temp. Phys. 110, 539 (1998); and private communications from M. Bienfait, J. K. Johnson, M. H. W. Chan, A. D. Migone and H. K. Kim.
-
-
-
Bienfait, M.1
Johnson, J.K.2
Chan, M.H.W.3
Migone, A.D.4
Kim, H.K.5
-
7
-
-
6444244907
-
-
A. Thess et al., Science 273 483 (1996).
-
(1996)
Science
, vol.273
, pp. 483
-
-
Thess, A.1
-
9
-
-
0011095441
-
-
G. Constabaris, J. R. Sams, Jr. and G. D. Halsey, Jr., J. Chem. Phys. 37, 915 (1962).
-
(1962)
J. Chem. Phys.
, vol.37
, pp. 915
-
-
Constabaris, G.1
Sams Jr., J.R.2
Halsey Jr., G.D.3
-
11
-
-
36749106046
-
-
R. Aziz, V. P. S. Nain, J. S. Carley, W. L. Taylor and G. T. McConville, J. Chem. Phys. 70, 4330 (1979). We omit substrate mediated interactions, which may be elastic or electromagnetic. For graphite, these are small. See F. Ancilotto and F. Toigo, Sol. St. Comm. 48, 593 (1983) and H. Y. Kim and M. W. Cole, Phys. Rev. B 35, 3990 (1987).
-
(1979)
J. Chem. Phys.
, vol.70
, pp. 4330
-
-
Aziz, R.1
Nain, V.P.S.2
Carley, J.S.3
Taylor, W.L.4
McConville, G.T.5
-
12
-
-
0020845250
-
-
R. Aziz, V. P. S. Nain, J. S. Carley, W. L. Taylor and G. T. McConville, J. Chem. Phys. 70, 4330 (1979). We omit substrate mediated interactions, which may be elastic or electromagnetic. For graphite, these are small. See F. Ancilotto and F. Toigo, Sol. St. Comm. 48, 593 (1983) and H. Y. Kim and M. W. Cole, Phys. Rev. B 35, 3990 (1987).
-
(1983)
Sol. St. Comm.
, vol.48
, pp. 593
-
-
Ancilotto, F.1
Toigo, F.2
-
13
-
-
0000076541
-
-
R. Aziz, V. P. S. Nain, J. S. Carley, W. L. Taylor and G. T. McConville, J. Chem. Phys. 70, 4330 (1979). We omit substrate mediated interactions, which may be elastic or electromagnetic. For graphite, these are small. See F. Ancilotto and F. Toigo, Sol. St. Comm. 48, 593 (1983) and H. Y. Kim and M. W. Cole, Phys. Rev. B 35, 3990 (1987).
-
(1987)
Phys. Rev. B
, vol.35
, pp. 3990
-
-
Kim, H.Y.1
Cole, M.W.2
-
16
-
-
0005027857
-
-
M. W. Cole and F. Toigo, Phys. Rev. B 23, 3914 (1981). Perfectly aligned tubes were considered (d = 9.95 Å), i.e. radial lines from z = 0 to the axis of each tube intersect the center of a hexagon.
-
(1981)
Phys. Rev. B
, vol.23
, pp. 3914
-
-
Cole, M.W.1
Toigo, F.2
|