Chemistry Letters Vol.35, No.3 (2006)
259
following scans.
Furthermore, the XP spectra obtained after the negative scan
to ꢁ1:25 V in a 0.1 M KOH solution showed the disappearance
of Pt4f and S2p peaks. These results clearly show that platinum
was removed with BDMT by the cathodic scan in alkaline solu-
tion, indicating that a Pt was not deposited on the Au(111) sur-
face but only on top of the SAM.
In summary, a novel method to construct a Pt/SAM/Au
sandwich structure without a short circuit between two metals
was proposed. XPS and electrochemical measurements con-
firmed that metallic platinum only deposited on top of the
SAM and that no metallic platinum existed on the Au(111) sur-
face. The metal deposition on Au underneath the SAM through
defect site was avoided because electrochemical deposition was
carried out in a platinum-ion free solution. In this way, no plat-
inum ions penetrated through imperfections in the course of
electrochemical reduction of Pt ions and only Pt ions pre-adsorb-
ed on the BDMT SAM were reduced.
Figure 2. Dependencies of relative intensities of (A) IPt=Ic and
(
B) Ipt=IAu on a take-off angle. IPt, IAu, and IC represent the
intensities of XP spectra of Pt 4f7=2, Au 4f7=2, and C1s peaks,
respectively.
electrode to determine the position of Pt. The relationship
between the relative intensities of Pt4f over Au4f and C1s and
the take-off angles was shown in Figure 2. The figure clearly
shows that the relative intensities of Pt4f to those of Au4f
and C1s increased as the take-off angle decreased. This proves
that Pt was indeed deposited not underneath but on top of the
BDMT SAM.
The results of electrochemical measurements also provide
evidence that the platinum layer formed only on top of the
SAM. A solid line in Figure 3 shows a current response when
the potential of the Pt–BDMT SAM-modified Au(111) electrode
was scanned negatively from 0 to ꢁ1:25 V. The cathodic current
increased significantly when the potential became more negative
than ꢁ1:0 V and a shoulder was observed at ꢁ1:18 V. The large
cathodic current is due to hydrogen-evolution reaction (HER)
and the shoulder is due to desorption of the Pt–BDMT SAM.
The reductive desorption took place at more negative potential
than the reductive desorption potential of the BDMT SAM
D. Qu acknowledges the Japan Society for the Promotion of
Science (JSPS) for a Postdoctoral Fellowship for foreign re-
searchers. Professor K. Shimazu is acknowledged for use of
the XPS. This work was partially supported by a Grant-in-Aid
for Scientific Research in the Priority Area of ‘‘Molecular Nano
Dynamics’’ (No. 16072202) from the Ministry of Education,
Culture, Sports, Science and Technology, Japan.
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