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Volumn 16, Issue 5, 2000, Pages 2220-2224

Influence of packing densities and surface order on the frictional properties of alkanethiol self-assembled monolayers (SAMs) on gold: A comparison of SAMs derived from normal and spiroalkanedithiols

Author keywords

[No Author keywords available]

Indexed keywords

ADSORPTION; ATOMIC FORCE MICROSCOPY; DENSITY (SPECIFIC GRAVITY); ELLIPSOMETRY; FRICTION; GOLD; INFRARED SPECTROSCOPY; MOLECULAR STRUCTURE; SULFUR COMPOUNDS; WETTING; X RAY PHOTOELECTRON SPECTROSCOPY;

EID: 0033906148     PISSN: 07437463     EISSN: None     Source Type: Journal    
DOI: 10.1021/la9909345     Document Type: Article
Times cited : (154)

References (35)
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    • Evaporated gold is polycrystalline with a predominant (111) orientation: Emch, R.; Nogami, J.; Dovek, M. M.; Lang, C. A.; Quate, C. F. J. Appl. Phys. 1989, 65, 79. Hallmark, V. M.; Chiang, S.; Rabolt, J. F.; Swalen, J. D.; Wilson, R. J. Phys. Rev. Lett. 1987, 59, 2879. Reichelt, K.; Lutz, H. O. J. Cryst. Growth 1971, 10, 103. Lee, M.-T.; Hsueh, C.-C.; Freund, M. S.; Ferguson, G. S. Langmuir 1998, 14, 6419.
    • (1989) J. Appl. Phys. , vol.65 , pp. 79
    • Emch, R.1    Nogami, J.2    Dovek, M.M.3    Lang, C.A.4    Quate, C.F.5
  • 14
    • 0011711484 scopus 로고
    • Evaporated gold is polycrystalline with a predominant (111) orientation: Emch, R.; Nogami, J.; Dovek, M. M.; Lang, C. A.; Quate, C. F. J. Appl. Phys. 1989, 65, 79. Hallmark, V. M.; Chiang, S.; Rabolt, J. F.; Swalen, J. D.; Wilson, R. J. Phys. Rev. Lett. 1987, 59, 2879. Reichelt, K.; Lutz, H. O. J. Cryst. Growth 1971, 10, 103. Lee, M.-T.; Hsueh, C.-C.; Freund, M. S.; Ferguson, G. S. Langmuir 1998, 14, 6419.
    • (1987) Phys. Rev. Lett. , vol.59 , pp. 2879
    • Hallmark, V.M.1    Chiang, S.2    Rabolt, J.F.3    Swalen, J.D.4    Wilson, R.J.5
  • 15
    • 0001568482 scopus 로고
    • Evaporated gold is polycrystalline with a predominant (111) orientation: Emch, R.; Nogami, J.; Dovek, M. M.; Lang, C. A.; Quate, C. F. J. Appl. Phys. 1989, 65, 79. Hallmark, V. M.; Chiang, S.; Rabolt, J. F.; Swalen, J. D.; Wilson, R. J. Phys. Rev. Lett. 1987, 59, 2879. Reichelt, K.; Lutz, H. O. J. Cryst. Growth 1971, 10, 103. Lee, M.-T.; Hsueh, C.-C.; Freund, M. S.; Ferguson, G. S. Langmuir 1998, 14, 6419.
    • (1971) J. Cryst. Growth , vol.10 , pp. 103
    • Reichelt, K.1    Lutz, H.O.2
  • 16
    • 0032179457 scopus 로고    scopus 로고
    • Evaporated gold is polycrystalline with a predominant (111) orientation: Emch, R.; Nogami, J.; Dovek, M. M.; Lang, C. A.; Quate, C. F. J. Appl. Phys. 1989, 65, 79. Hallmark, V. M.; Chiang, S.; Rabolt, J. F.; Swalen, J. D.; Wilson, R. J. Phys. Rev. Lett. 1987, 59, 2879. Reichelt, K.; Lutz, H. O. J. Cryst. Growth 1971, 10, 103. Lee, M.-T.; Hsueh, C.-C.; Freund, M. S.; Ferguson, G. S. Langmuir 1998, 14, 6419.
    • (1998) Langmuir , vol.14 , pp. 6419
    • Lee, M.-T.1    Hsueh, C.-C.2    Freund, M.S.3    Ferguson, G.S.4
  • 28
    • 0032495430 scopus 로고    scopus 로고
    • Calibration curves were constructed for Au by plotting ln(Au 4f) versus the effective number of carbons and treating the attenuation due to the sulfur atom as equivalent to 1.5 methylene units (Harder, P.; Grunze, M.; Dahint, D.; Whitesides, G. M.; Laibinis, P. E. J. Phys. Chem. B 1998, 102, 426).
    • (1998) J. Phys. Chem. B , vol.102 , pp. 426
    • Harder, P.1    Grunze, M.2    Dahint, D.3    Whitesides, G.M.4    Laibinis, P.E.5
  • 30
    • 0000992383 scopus 로고
    • 21 Au intensities, however, scale linearly with chain length and can consequently be used to reliably determine packing densities (Laibinis, P. E.; Bain, C. D.; Whitesides, G. M. J. Phys. Chem. 1991, 95, 7017). Therefore, the packing densities obtained from the C 1s signals should be regarded as approximations under the aforementioned assumption and are provided only in support of the packing densities determined from the Au 4f signals.
    • (1991) J. Phys. Chem. , vol.95 , pp. 7017
    • Laibinis, P.E.1    Bain, C.D.2    Whitesides, G.M.3
  • 31
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    • note
    • Errors in the reported packing densities were determined by propagating the errors associated with the measured C 1s and Au 4f intensities (2% for C 1s and 1% for Au 4f, which were determined from the average and standard deviation of four measurements) throughout the calculations.


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