The formation of CuSeCN on a copper anode was studied in 0.1 and 0.5 m
ol dm(-3) KSeCN solutions. A thin film of polycrystalline CuSeCN was p
roduced with a midpoint potential between the anodic and cathodic peak
s for 0.1 mol dm(-3) KSeCN at -0.253 V, close to the open-circuit pote
ntial of -0.249 V. A precursory anodic peak or shoulder was seen at ab
out -0.210 V, and was ascribed to the formation of a primary (barrier)
film. The anodic peak currents for the primary film were linearly dep
endent upon the sweep rate. Potential steps into the primary film regi
on produced current transients, with the current decaying in proportio
n to the reciprocal of time. The anodic peak current and potential for
the secondary polycrystalline film were proportional to the square ro
ot of the sweep rate, an effect which is consistent with a model for p
orous film growth controlled by the resistance across the underlying b
arrier film. A weak Raman band due to Se-bonded CuSeCN at 2164 cm(-1)
was also observed in situ.