Indirect e-beam evaporation of metal on a cooled substrate that allows making reproducible and gentle electrical contact to molecular films of organic molecules yields strikingly different results with Pd and Au. This is attributed to different growth modes of the metals, which lead to different molecule/metal interactions and to Au penetration in between the molecules. These differences can radically change the effect of the molecules on the resulting junctions.

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6.

The dipole layer effect operates at both forward and reverse bias, as explained in Ref. 3 (cf. Fig. 1 in that reference).

7.
The differences in shapes of the ln(I)V curves between the Pd and Au junctions [Figs. 1(a) and 1(b)] as well as the higher series resistance with Au, than with Pd, can be ascribed to the differences in metal film growth as described in the text. These lead to effective contact areas that, although still larger than the geometrical ones, are smaller with Au than with Pd, as well as to different densities of interface states [cf.
D. R.
Heslinga
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H. H.
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D. P.
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T. M.
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This interpretation is supported by low frequency capacitance–voltage (CV) measurements (unpublished).
8.

The molecular dipole is taken as positive if the negative pole of the dipole points away from the binding group, viz. away from the surface after binding. As negative dipoles we used dCOCH3(4.4D), dCCH3(4.0D) and dCH(3.5D) and as positive dipoles we used dCCN(+2.3D) and dCCF3(+2.7D). All values (in parentheses) are in Debye units, for the free molecules.

9.
The difference in BHs of the bare PdGaAs and AuGaAs junctions can be ascribed to different pinning defects at their interfaces [cf.
T.
Drummond
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59
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and/or hydrogenation effects [cf.
H. Y.
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32
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14.

Complementary experiments showed ICICE-made contacts to have higher effective than geometrical areas, whereas the effective LOFO-made junction areas are up to an order of magnitude smaller. As is clear from Refs. 1 and 3, the larger the effective contact area between deposited metal and molecules, the higher the dipole density due to the interaction of the metal spill-over electron density with the molecules, which is the dipole density that dictates the BH-CPDL trend for junctions with LOFO-made contacts and with ICICE-made Pd ones.

15.
The systematic effect of the molecules shown in Fig. 1, supported by TOF SIMS and XPS experiments, imply the absence of significant chemical interactions between the functional groups used here and the evaporated metals, even though different functional groups may lead to (minor) differences in the growth mode of the metal, on top of the dC–X films, as was shown recently for mono- and di-thiol conjugated molecules [cf.
B.
de Boer
,
M. M.
Frank
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Y. J.
Chabal
,
W.
Jiang
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E.
Garfunkel
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Z.
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20
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1539
(
2004
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16.
Near-full coverage was obtained by adsorbing benzoic acid molecules [cf.
S.
Bastide
,
R.
Butruille
,
D.
Cahen
,
A.
Dutta
,
J.
Libman
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A.
Shanzer
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L.
Sun
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A.
Vilan
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J. Phys. Chem. B
101
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2678
(
1997
)]
on GaAs, after adsorbing dicarboxylic acids [cf. also
D. G.
Wu
,
D.
Cahen
,
P.
Graf
,
R.
Naaman
,
A.
Nitzan
, and
D.
Shvarts
,
Chem.-Eur. J.
7
,
1743
(
2001
)]. Adsorption of only benzoic acids gave BH-CPDL trends as did adsorption of only dC–X molecules.
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