Replacing Ag<sup>TS</sup>SCH<sub>2</sub>‐R with Ag<sup>TS</sup>O<sub>2</sub>C‐R in EGaIn‐Based Tunneling Junctions Does Not Significantly Change Rates of Charge Transport — Kung‐Ching Liao (2014) | RDL Network
Replacing Ag<sup>TS</sup>SCH<sub>2</sub>‐R with Ag<sup>TS</sup>O<sub>2</sub>C‐R in EGaIn‐Based Tunneling Junctions Does Not Significantly Change Rates of Charge Transport
Article 2014 en
Authors
KL
Kung‐Ching Liao
HY
Hyo Jae Yoon
CB
Carleen M. Bowers
Abstract
1 min read
Abstract This paper compares rates of charge transport by tunneling across junctions with the structures Ag TS X(CH 2 ) 2 n CH 3 //Ga 2 O 3 /EGaIn ( n =1–8 and X= SCH 2 and O 2 C); here Ag TS is template‐stripped silver, and EGaIn is the eutectic alloy of gallium and indium. Its objective was to compare the tunneling decay coefficient ( β , Å −1 ) and the injection current ( J 0 , A cm −2 ) of the junctions comprising SAMs of n ‐alkanethiolates and n ‐alkanoates. Replacing Ag TS SCH 2 ‐R with Ag TS O 2 C‐R (R=alkyl chains) had no significant influence on J 0 (ca. 3×10 3 A cm −2 ) or β (0.75–0.79 Å −1 )—an indication that such changes (both structural and electronic) in the Ag TS XR interface do not influence the rate of charge transport. A comparison of junctions comprising oligo(phenylene)carboxylates and n ‐alkanoates showed, as expected, that β for aliphatic (0.79 Å −1 ) and aromatic (0.60 Å −1 ) SAMs differed significantly.
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