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Tunneling through the Schottky barrier would occur only at strong reverse bias, a voltage regime not accessed and studied here.
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A change in GaAs surface pre-treatment yields data that are even closer to those obtained for the Si systems (see ref 9).
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The effective dielectric constant changes by 10-15% over this temperature range (ref 53), insufficient to explain by itself the observed temperature dependence.
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The reason for the linearity of the plots at higher bias is discussed elsewhere (ref 50).
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The same behaviour was observed with other molecular junctions having different metallic top contact and different molecular length
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The same behaviour was observed with other molecular junctions having different metallic top contact and different molecular length.
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2 relates to the fact that tunneling is temperature-independent only to a first approximation. The actual temperature dependence is due to the change in the electrode's electronic carrier density around the Fermi level (near the conduction band minimum or valence band maximum for a semiconductor) and in the electrode's Fermi level position with temperature (see also refs 50, 48).
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2 relates to the fact that tunneling is temperature-independent only to a first approximation. The actual temperature dependence is due to the change in the electrode's electronic carrier density around the Fermi level (near the conduction band minimum or valence band maximum for a semiconductor) and in the electrode's Fermi level position with temperature (see also refs 50, 48).
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