to leave a regular array of interconnected spherical voids. The
size of these voids is determined by the size of the polystyrene
latex particles used. Since polystyrene latex particles of tightly
controlled size distribution are readily commercially available
in sizes from 0.05 to 90 mm the size of the voids can be readily
controlled. Control over the quantity of charge passed in the
electrochemical deposition of the film allows control over the
final film thickness. Thus this method represents a simple route
to the production of ordered macroporous films of metals, metal
alloys, and polymers with potentially interesting and useful
photonic, catalytic, magnetic, or other properties.
We thank the Embassy of the Arab Republic of Egypt,
Educational and Cultural Bureau, London for their support of
Mohamed A. Ghanem. We also thank Alastair Clark for
assistance in obtaining the SEM images and manufacture of the
gold substrates.
Notes and references
† Experimental: Cobalt acetate [Co(Ac)2·4H2O, 99.5%] and potassium
acetate (KAc, 99.4%) were obtained from Fluka. Hexachloroplatinic acid
and diammonium tetrachloropalladate were obtained from Aldrich (purity
99.99%). 0.5 wt% suspensions of 0.40 and 1.00 mm diameter polystyrene
latex spheres in water were obtained from Agar Scientific, 2.5 wt%
suspensions of 0.70 mm diameter polystyrene latex spheres in water were
obtained from Alfa Asear. The working electrodes were prepared by
evaporating 10 nm of a chromium adhesion layer followed by 200 nm of
gold onto thin glass microscope slides. A large area platinum gauze was
used as the counter electrode and home made saturated calomel (SCE) as the
reference electrode. Before use, the gold working electrodes were sonicated
in propanol for 1 h and then rinsed with deionised water. A volume of ca.
0.3 cm3 of the suspension of polystyrene latex spheres diluted with water to
0.5 wt% was spread over ca. 1 cm2 area of the gold electrode and allowed
to dry slowly over 2 d in a controlled humidity chamber. The working
electrode, together with the adherent, dry, polystyrene latex bead template,
was dipped in to the appropriate electrolyte solution to deposit the metal
film. The deposition solutions were either 50 mmol dm23 H2PtCl6, 40 mol
dm23 (NH4)2PdCl4, or 0.1 mol dm23 Co(Ac)2 with 0.1 mol dm23 KAc. The
deposition was carried out potentiostatically at potentials of 0.10, 0.25 or
20.90 V vs. SCE for the electrochemical deposition of platinum, palladium,
or cobalt. After deposition the polystyrene latex spheres were dissolved out
of the metal films by soaking in toluene for 24 h.
Fig. 2 Scanning electron micrographs of macroporous films of platinum,
palladium and cobalt electrochemically deposited, at potentials of 0.10, 0.25
and 20.90 V vs. SCE respectively, through templates formed using
polystyrene latex spheres pre-assembled on gold electrode surfaces. (a)
Platinum film, deposition charge 22.00 C cm22, polystyrene latex sphere
diameter 0.40 mm; (b) cobalt film, deposition charge 21.40 C cm22
,
polystyrene latex sphere diameter 0.40 mm; (c) cross-sectional image of a
platinum film, deposition charge 21.50 C cm22, polystyrene latex sphere
diameter 0.40 mm; (d) palladium film, deposition charge 21.15 C cm22
polystyrene latex sphere diameter 0.70 mm.
,
periodic hexagonal array of monodisperse pores. The pore to
pore centre separation in this case was 770 ± 10 nm (n = 30).
Fig. 1(d) shows a cross sectional image of a platinum film
prepared by deposition of 21.00 C cm22 through a template of
0.40 mm polystyrene latex spheres. The formation of a
monolayer of spherical pores embedded in the platinum film
(which in this case was grown to a thickness of approximately
0.4 mm) can be clearly seen.
Figs. 2(a) and 2(b) show scanning electron micrographs of
thicker films of platinum and cobalt where sufficient charge has
been passed to deposit films several multiples of the polystyrene
latex sphere diameter in thickness. The micrographs show that
the spherical pores left in the platinum or cobalt films after
removal of the polystyrene latex spheres are arranged in a well
ordered three dimensional hexagonal close packed structure. In
addition, the connections between the spherical voids within the
film, formed where the polystyrene latex spheres in one layer
were in contact with those in the underlayer, can be seen as the
three dark areas within each pore. In Fig. 2(a) the mouths of the
pores have a rounded triangular shape. This appears to be a
regular feature of films which are grown to a thickness
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