237
close to IUPAC type I classification13 but has a slight shoulder
below the relative pressure of 0.15, suggesting that the pore size
is in an intermediate range between micropore and mesopore
regions. The average pore sizes calculated based on Barrett-
Joyner-Halenda (BJH) theory13 and nonlinear density functional
theory (NLDFT)14 are 1.5 and 2.2 nm, respectively (Table S1).12
Note that BJH theory tends to underestimate the pore size in the
miropore region.15 The BET surface area and pore volume are
increase of pore size is relatively facile, e.g., by using swelling
agent or block copolymers, the generation of well-regulated
small pores is still difficult.16,17 In this context, the tricationic
surfactant used in this study provides a promising method.
Further decrease of the pore size can be achieved by reducing the
length of the alkylene spacers. When B-C6TMA having C6
spacers was used as template, only a broad peak was observed
by XRD (data not shown); however, the pore size was greatly
decreased to 1.1 nm, as evaluated by NLDFT (BJH theory is no
more applicable for such a small pore).
In conclusion, a novel rigid-core surfactant consisting of
three trimethylammonium heads attached to a benzene core via
flexible hydrocarbon chains was examined as a template for
synthesizing ordered porous silica. This surfactant was effective
for generating small and regularly arranged pores, which is
attributed to its strong tendency to form cylindrical assemblies.
The synthesis of such ordered porous silica with small
mesopores is of both scientific and practical importance.
¹1
calculated to be 870 m2 g and 0.5 cm3 g¹1, respectively.
To clarify the specific properties of B-C10TMA, decyltri-
methylammonium bromide (C10TMA) was also examined as
template. A control experiment was performed at the molar
ratios of 1TEOS:0.4NaOH:140H2O:0.06C10TMA under other-
wise identical conditions. In contrast to the highly ordered pore
structure achieved with B-C10TMA, the sample prepared with
C10TMA is less ordered, exhibiting broader peaks in the
XRD pattern (Figure 1, right, a). A lower BET surface area
(360 m2 g¹1) is also confirmed. These results are consistent with
the fact that it is generally difficult to obtain highly ordered
porous silica using alkyltrimethylammonium surfactants with
short alkyl chains containing less than 12 carbons, due to
hydrophobic interaction poorer than the electric repulsion
between cationic head groups.16,17 Thus, the rigid benzene core
of B-C10TMA should play a crucial role in the formation of
highly ordered structure.
UV-vis spectroscopy indicates ³-³ stacking of benzene
cores in the silica-B-C10TMA composites18 (Figure S4). The
absorption bands of the composites are red-shifted compared to
those of the simple mixture of silica powder and B-C10TMA.
Such ³-³ stacking in addition to the hydrophobic interactions
of B-C10TMA should stabilize the silica-surfactant composite
mesophase. It is plausible that B-C10TMA molecules are
stacked to form cylindrical micelles where the side chains
radiate outward from the central benzene cores (Scheme 1c).
This model is supported by the experimental result that the
expansion of the micelle diameter hardly occurred even by
adding TMB, a typical swelling agent. In general, the d10
spacing is increased by the addition of hydrophobic swelling
agents5 when conventional surfactants like C10TMA are used
as template; however, such a behavior was not observed for
B-C10TMA (Figure 1b).
In the silica-B-C10TMA mesophase, a trisubstituted ben-
zene core should be rotated to some degree from the adjacent
core to minimize the steric repulsion between alkylene spacers.
It appears that the alkylene spacers are not in a fully extended
state, because the pore size of the calcined sample is much
smaller than the molecular size of B-C10TMA with all-trans
alkylene spacers (ca. 3.8 nm). Note that cationic head groups
do not thrust into silica walls, unlike nonionic surfactants
which penetrate silica walls and produce micropores. It is also
interesting that despite the presence of the benzene core (ca.
0.7 nm in diameter, including ether oxygen atoms), the pore size
is slightly smaller than that templated with C10TMA (1.6 nm).12
This can be explained by the low number density of trimethyl-
ammonium(alkyl) groups in the silica-B-C10TMA composite.
In fact, the N/Si ratio calculated by combination of CHN
analysis and thermogravimetry was 0.18, which is lower than for
the sample prepared with C10TMA (0.20).
This work was supported in part by a Grant-in-Aid for
Scientific Research (B) from the Japan Society for the Promotion
of Science. This work was partly conducted in the Center for
Nano Lithography & Analysis, The University of Tokyo,
supported by the Ministry of Education, Culture, Sports, Science
and Technology, Japan. We thank Prof. Kazunari Domen at the
University of Tokyo for UV-vis measurements.
References and Notes
1
2
3
S. Manne, T. E. Schäffer, Q. Huo, P. K. Hansma, D. E. Morse,
A. E. Garcia-Bennett, S. Williamson, P. A. Wright, I. J.
D. Y. Zhao, Q. Huo, J. Feng, J. Kim, Y. Han, G. D. Stucky,
4
5
6
7
S. Shen, A. E. Garcia-Bennett, Z. Liu, Q. Lu, Y. Shi, Y. Yan, C.
8
9
M. Kimura, K. Wada, K. Ohta, K. Hanabusa, H. Shirai, N.
12 Supporting Information is available electronically on the
index.html.
13 S. Brunauer, L. S. Deming, W. E. Deming, E. Teller, J. Am.
14 P. I. Ravikovitch, D. Wei, W. T. Chueh, G. L. Haller, A. V.
16 R. Ryoo, I.-S. Park, S. Jun, C. W. Lee, M. Kruk, M. Jaroniec,
17 J. S. Beck, J. C. Vartuli, G. J. Kennedy, C. T. Kresge, W. J.
18 A. R. A. Palmans, J. A. J. M. Vekemans, E. E. Havinga, E. W.
Pore size control of surfactant-templated and ordered porous
silica is important from a practical viewpoint. Although the
Chem. Lett. 2010, 39, 236-237
© 2010 The Chemical Society of Japan