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Harten, U.; Lahee, A. M.; Toennies, J. P.; Woll, Ch. Phys. Rev. Lett. 1985, 54, 2619. Woll, Ch.; Chiang, S.; Wilson, R. J.; Lippel, P. H. Phys. Rev. B 1989, 39, 7988.
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19
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11644279794
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note
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The vapor of hexanethiol was introduced onto the Au(111) surfaces via a variable leak valve with a nozzle (hole diameter, 0.5 mm; nozzle length, 200 mm; distance from sample, 10 mm). Here, since the local pressure at the sample position during the exposure could not be precisely calibrated, we use readings of a pressure gauge located 200 mm underneath the sample as apparent gas pressures.
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20
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11644284610
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To be submitted
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At 0.5 langmuirs, a small amount of herringbone-like features still remain on the surface, and these features completely disappear at slightly higher exposures (0.6 langmuirs). Surface areas other than the herringbone-like features and striped islands are filled with obscure domains, which we attributed to a "2D liquid" phase since these domains have no ordered structure and their domain boundaries are fluctuating. The details of the growth processes will be reported elsewhere. Kondoh, H.; Kodama, C.; Sumida, H.; Nozoye, H. To be submitted.
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Kondoh, H.1
Kodama, C.2
Sumida, H.3
Nozoye, H.4
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21
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0000788117
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Lin, J.-L.; Bent, B. E. J. Am. Chem. Soc. 1993, 115, 2849; J. Phys. Chem. 1993, 97, 9713.
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J. Am. Chem. Soc.
, vol.115
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Lin, J.-L.1
Bent, B.E.2
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22
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0001291439
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Lin, J.-L.; Bent, B. E. J. Am. Chem. Soc. 1993, 115, 2849; J. Phys. Chem. 1993, 97, 9713.
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(1993)
J. Phys. Chem.
, vol.97
, pp. 9713
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24
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11644285163
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note
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Annealing of the high-density phases (i.e., the disordered phase and the c(4 × 2) phase) results in transformation to the striped phase via partial desorption of the surface thiolates. TD spectra for the high-density phases also exhibit desorption features associated with the thiolate radicals at around 510 K, which is probably due to the structure transformation during the TDS ramp.
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