Chemistry Letters Vol.33, No.11 (2004)
1409
of the copolymer. The film thickness was about 30 nm, which
was double of the monolayer films. On the basis of the FE-
SEM observations (see Supplemental Information, Figures S2),
we suggest that the porous structure of this film is the same as
that of the monolayer nanoporous films. In the nanoporous films
with five and eight layers of nanopores, the nanopores at the
film-substrate interface are hemispheric in shape and the silica
pillars adhere to the substrate.18 In contrast, in the mono- and
double-layered films, the silica layer adheres to the substrate.
The thin copolymer layer may allow rapid permeation of the
TEOS and a high mobility of the silicate-copolymer composite
film formed at the film-substrate interface. The thermal conduc-
tivity of the double-layer nanoporous silica film (containing the
copolymer) was 0:174 ꢁ 0:007 W mꢂ1 Kꢂ1, a level which was
lower than that of the bulk silica. The measurements were car-
ried out at 25 ꢃC in vacuum (<0:02 Pa). After calcination, the
thermal conductivity was decreased by 70% (0:125 ꢁ 0:005
W mꢂ1 Kꢂ1).
pores should perform very well as nanodevices and nanoflasks.
We gratefully acknowledge the assistance of the GHAS
laboratory and Mr. M. Kawashima of Osaka University for the
FE-SEM measurements.
References and Notes
1
2
3
4
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Figure 4 shows the ultrathin silica films obtained by spin
coating synthesis. The periodicity of the nanopores was poor al-
though three or four layers of nanopores were observed. It was
difficult to fabricate silica films with less than three layers by
the spin coating synthesis method.
10 Q. Huo, R. Leon, P. M. Petroff, and G. D. Stucky, Science, 268,
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(1996).
Surface of the silica film
Surface of the substrate
14 Y. Lu, R. Ganguli, C. A. Drewien, M. T. Anderson, C. J. Brinker,
W. Gong, Y. Guo, H. Soyez, B. Dunn, M. H. Huang, and J. I. Zink,
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S. M. Han, and C. J. Brinker, J. Am. Chem. Soc., 125, 11646 (2003).
17 N. Nishiyama, S. Tanaka, Y. Egashira, Y. Oku, and K. Ueyama,
Chem. Mater., 15, 1006 (2003).
Section of the silicon substrate
60 nm
Figure 3. FE-SEM image of the cross-section of an ultrathin
silica film with double-layer of nanopores. The film was pre-
pared by vapor phase synthesis.
18 S. Tanaka, N. Nishiyama, Y. Egashira, Y. Oku, and K. Ueyama,
J. Am. Chem. Soc., 126, 4854 (2004).
19 We fabricated ultrathin nanoporous silica films by vapor phase and
spin coating synthesis. Vapor phase synthesis: Nonionic amphiphilic
triblock copolymer Pluronic F127 (EO106PO70EO106) was used as a
templating agent. A precursor solution of 0.05 g of Pluronic F127,
9.2 g of ethanol, and 3.6 g of deionized water was dropped onto a sil-
icon substrate (5 ꢄ 5-cm piece), and then the substrate was spun at a
rate of up to 4000 rpm for 1 min using a SPINCOATER 1H-DX2
(Mikasa Co.). Next, the triblock copolymer film was placed vertical-
ly in a closed vessel (200 cm3) along with a separate, small amount of
TEOS and HCl (5 N). The vessel was then placed in an oven at 90 ꢃC.
Thus, the copolymer film was exposed to a saturated TEOS vapor
under autogenous pressure. Removal of the copolymer template from
the composite was subsequently carried out by calcination at 400 ꢃC
in air for 5 h with a heating rate of 1 ꢃC/min. Spin coating synthesis:
A precursor solution of TEOS, Pluronic F127, ethanol, and deionized
water was spin-coated on a silicon substrate. The film thickness was
controlled by adjustment of the spinning rate and the concentrations
in the precursor solution.
Surface of the silica film
Section of the silicon substrate
60 nm
Figure 4. FE-SEM image of the cross-section of an ultrathin
silica film with about four layers of nanopores. The film was ob-
tained by spin coating synthesis.
20 FE-SEM images were recorded on a Hitachi S-5000L microscope at
an acceleration voltage of 21 kV. The samples were not coated before
the FE-SEM measurements. The ordered structure of the films was
investigated with a Philips X’ Pert-MPD diffractometer using Cu Kꢀ
In conclusion, we have successfully fabricated, by vapor
phase synthesis, ultrathin silica films with a monolayer of uni-
form nanopores. We were able to control the number of layers
via changes in the triblock copolymer concentration in the pre-
cursor solution. Such ultrathin films with a monolayer of nano-
ꢀ
radiation with ꢁ ¼ 1:5418 A. The copper anode was operated at 40
kV and 30 mA. The peak evolution was followed in the ꢂ/2ꢂ
Bragg–Brentano scattering geometry, 2ꢂ varying from 0.2 to 8
degrees, with a step size of 0.01 degree and a time per step of 1.0 s.
Published on the web (Advance View) September 29, 2004; DOI 10.1246/cl.2004.1408