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11
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Smith, R.S.1
Huang, C.2
Wong, E.K.L.3
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14
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36449006776
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Hage, W.1
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10244270976
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W. Hage, A. Hallbrucker, E. Mayer, and G. P. Johari, J. Chem. Phys. 103, 545 (1995).
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Hage, W.1
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Johari, G.P.4
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17
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0030284533
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P. Löfgren, P. Ahlström, D. V. Chakarov, J. Lausmaa, and B. Kasemo, Surf. Sci. 367, L19 (1996).
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Kasemo, B.5
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19
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0038879643
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Z. Dohnálek, R. L. Ciolli, G. A. Kimmel, K. P. Stevenson, R. S. Smith, and B. D. Kay, J. Chem. Phys. 110, 5489 (1999).
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Dohnálek, Z.1
Ciolli, R.L.2
Kimmel, G.A.3
Stevenson, K.P.4
Smith, R.S.5
Kay, B.D.6
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20
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85037499550
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note
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The Knudsen number (ratio of gas mean free path and nozzle diameter), Kn, of our water beam source is ∼0.1, which falls into the transition range between effusive (Kn≥1) and supersonic (Kn<0.01) beams. The beam properties are close to that of effusive beams having nearly thermal velocity distribution and no clustering.
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-
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21
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0033525818
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K. P. Stevenson, G. A. Kimmel, Z. Dohnálek, R. S. Smith, and B. D. Kay, Science 283, 1505 (1999).
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(1999)
Science
, vol.283
, pp. 1505
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Stevenson, K.P.1
Kimmel, G.A.2
Dohnálek, Z.3
Smith, R.S.4
Kay, B.D.5
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23
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0001491673
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R. J. Speedy, P. G. Debenedetti, R. S. Smith, C. Huang, and B. D. Kay, J. Chem. Phys. 105, 240 (1996).
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(1996)
J. Chem. Phys.
, vol.105
, pp. 240
-
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Speedy, R.J.1
Debenedetti, P.G.2
Smith, R.S.3
Huang, C.4
Kay, B.D.5
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24
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0000371261
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R. S. Smith, C. Huang, E. K. L. Wong, and B. D. Kay, Phys. Rev. Lett. 79, 909 (1997).
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(1997)
Phys. Rev. Lett.
, vol.79
, pp. 909
-
-
Smith, R.S.1
Huang, C.2
Wong, E.K.L.3
Kay, B.D.4
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28
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0033525818
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2O molecules was varied [K. P. Stevenson, G. A. Kimmel, Z. Dohnálek, R. S. Smith, and B. D. Kay, Science 283, 1505 (1999)], in agreement with predictions from ballistic deposition models [A. L. Barabasi and H. E. Stanley, Fractal Concepts in Surface Growth (Cambridge University Press, Cambridge, 1995); H. van Kranenburg and C. Lodder, Mater. Sci. Eng., R. 11, 295 (1994)].
-
(1999)
Science
, vol.283
, pp. 1505
-
-
Stevenson, K.P.1
Kimmel, G.A.2
Dohnálek, Z.3
Smith, R.S.4
Kay, B.D.5
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29
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0003431520
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Cambridge University Press, Cambridge
-
2O molecules was varied [K. P. Stevenson, G. A. Kimmel, Z. Dohnálek, R. S. Smith, and B. D. Kay, Science 283, 1505 (1999)], in agreement with predictions from ballistic deposition models [A. L. Barabasi and H. E. Stanley, Fractal Concepts in Surface Growth (Cambridge University Press, Cambridge, 1995); H. van Kranenburg and C. Lodder, Mater. Sci. Eng., R. 11, 295 (1994)].
-
(1995)
Fractal Concepts in Surface Growth
-
-
Barabasi, A.L.1
Stanley, H.E.2
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30
-
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0028256906
-
-
2O molecules was varied [K. P. Stevenson, G. A. Kimmel, Z. Dohnálek, R. S. Smith, and B. D. Kay, Science 283, 1505 (1999)], in agreement with predictions from ballistic deposition models [A. L. Barabasi and H. E. Stanley, Fractal Concepts in Surface Growth (Cambridge University Press, Cambridge, 1995); H. van Kranenburg and C. Lodder, Mater. Sci. Eng., R. 11, 295 (1994)].
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(1994)
Mater. Sci. Eng., R.
, vol.11
, pp. 295
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-
Van Kranenburg, H.1
Lodder, C.2
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32
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0029507484
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B. S. Berland, D. E. Brown, M. A. Tolbert, and S. M. George, Geophys. Res. Lett. 22, 3493 (1995).
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(1995)
Geophys. Res. Lett.
, vol.22
, pp. 3493
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Berland, B.S.1
Brown, D.E.2
Tolbert, M.A.3
George, S.M.4
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35
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0031384692
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The bilayer spacing is calculated using a nearest-neighbor distance of 2.75 Å and a tetrahedral arrangement of nearest-neighbor molecules
-
M. A. Zondlo, T. B. Onasch, M. S. Warshawsky, and M. A. Tolbert, J. Phys. Chem. B 101, 10887 (1997). The bilayer spacing is calculated using a nearest-neighbor distance of 2.75 Å and a tetrahedral arrangement of nearest-neighbor molecules.
-
(1997)
J. Phys. Chem. B
, vol.101
, pp. 10887
-
-
Zondlo, M.A.1
Onasch, T.B.2
Warshawsky, M.S.3
Tolbert, M.A.4
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