B.-L. Su, X.-Y. Yang, Z.-M. Liu et al.
designated MMM(0), MMM(1), and MMM(2), respective-
ly). The precursor material exhibits a macroscopic network
with relatively homogenous and straight channel-shaped
macropores of 2–5 mm in diameter. The macrochannels are
arranged parallel to each other (Figure 2A and B). The
walls around the macrochannels are composed of very ho-
mogenous particles of about 150 nm in size (Figure 2B and
C and inset), which result in interparticle porosity. These
particles are themselves formed by aggregation of smaller
nanoparticles (Figure 2C and inset) and thus have accessible
smaller mesovoids, similar to previously reported meso–
macroporous materials.[36] As the reaction time proceeded
(1 d), material MMM(1) retained its meso–macroporous
structure (Figure 2D–F) and zeolite MFI nanoparticles
began to form on the macropore walls (Figure 2F, Fig-
ure 3A). The dark-field TEM image (Figure 3B) was ac-
quired on the same region as the bright-field TEM image
(Figure 3A). The bright spots in the image correspond to
MFI nanocrystals (Figure 3B). Figure 3C shows the wall
separating two macrochannels. The crystalline zone and the
remaining amorphous phase are easily distinguishable. The
nanocrystals that developed around the macropore walls
gradually embedded themselves within the continuous amor-
phous inorganic matrix and thus formed a new crystalline
framework while preserving the meso- and macroporous
scaffold (Figure 3A–C). These zeolite MFI particles, located
within the framework of the meso–macroporous aluminosili-
cate precursor (Figure 2G–I, Figure 3D) became more crys-
talline after 2 d at 1308C. Notably, the bright-field image
(Figure 3D) showed that the amorphous phase of the initial
material had been completely replaced by the nanocrystals
and thus suggests that this process aided the crystallization
of the amorphous framework leading to a micro–meso–mac-
roporous aluminosilicate structure. Crystallization or the
transformation of amorphous aluminosilicate phase into
well-crystallized zeolite phase did not affect the meso–mac-
roporous framework of the precursor (Figure 2G and H).
The parallel macrochannel structure is well preserved. The
dark-field image (Figure 3E) further indicated that the
meso–macroporous framework was mainly crystalline, owing
to the presence of bright spots corresponding to the MFI
nanocrystals fully occupying the matrix. Figure 3F shows an
image of the wall separating two macrochannels, which is
clearly composed of an assembly of nanocrystals. In addi-
tion, higher-magnification TEM images (Figure 3F and G)
and circular streaking in the electron diffraction pattern
(inset of Figure 3G) indicated that the micro–meso–macro-
porous aluminosilicates were constructed from randomly
oriented zeolite nanocrystals. Furthermore, high-resolution
(HR) TEM studies (Figure 3G–I, H and I) confirm that the
sample has very uniform nanocrystals with high crystallinity
observed by SEM (Figure 2G). The ZSM-5 nanoparticles in
the macroporous wall of MMM(3) show a high degree of
crystallinity, and the lattice fringes of 0.892 (Figure 3H) and
0.996 nm (Figure 3I) correspond to the (210) and (200) crys-
tal planes of the tetragonal structure of ZSM-5 (JCPDS card
no. 044-0002), respectively. Electron microscopy investiga-
tion revealed that the amorphous domain gradually disap-
peared with increasing reaction time, and subsequently
larger mesopores and voids, compared to the initial meso-
pores, were generated. Owing to the effect of the structure-
directing agent TPA+, the microporous zeolite crystals were
able to grow by using the amorphous phase as a source of
aluminum and silicon atoms to create new mesostructure.
Interestingly, the entirely zeolite architecture exhibits a uni-
form zeolite crystal size of about 150 nm (Figure 2I and Fig-
ure 3D, F–I), and this results in relatively uniform meso-
pores or mesovoids, which lead to improved catalytic activi-
ty. The crystal size of 150 nm is approximately the same size
as that of the amorphous aggregate of nanoparticles found
in the precursor material (ca. 150–200 nm, see Figure 2C).
Moreover, TEM studies (Figure 3C and F) reveal that the
nanocrystals of the surface of the macroporous channels did
not grow excessively with increasing reaction time, while the
crystal size remained around 150 nm. This phenomenon is
unique, and quite different from other routes reported pre-
viously.[24–25,43–50] As the size of the microporous zeolite crys-
tal formed is similar to that of the starting amorphous aggre-
gate of nanoparticles, this could potentially indicate that
each aggregate of nanoparticles was transformed into a zeo-
lite crystal, possibly due to good accessibility for the struc-
ture-directing agent and supplementary silica source of the
unique mesostructure formed by aggregation of the nano-
particle precursor and the relatively mild glycerol system.
This is probably a critical factor in the formation of uniform
crystals and maintenance of the mesostructure. The macro-
porous structure was also unaffected due to the relatively
thick macroporous wall in the meso–macroporous alumino-
silicate and relatively mild reaction system (Figures 2G–I
and 3B–F). This indicates that the overall meso–macropo-
rous structure within the initial material was maintained
during the transformation (Figures 2 and 3). Furthermore,
even after calcination at 5508C for 5 h, the nanocrystals in
macroporous walls do not obviously aggregate with each
other, and thus the mesopores or mesovoids are not affected
(Figure 3). This means that the hierarchical materials have
highly thermal stability, which is mostly important for recy-
cling. In summary these observations clearly suggest that a
hierarchically micro–meso–macroporous material which has
well-defined macropores and interconnecting mesopores
within the macropore walls was constructed from zeolite
nanocrystals with tunable micropores.
Figure 4 shows XRD patterns of micro–meso–macropo-
rous aluminosilicates MMM(0), MMM(1), and MMM(2)
synthesized at 1308C. Notably, the peaks in the XRD pat-
terns of samples MMM(1) and MMM(2) are characteristic
of ZSM-5 crystal symmetry (JCPDS card no. 044-0002), and
the enhanced wide-angle XRD pattern suggested that the
degree of crystallinity gradually increased and the amor-
phous phase of the precursor gradually disappeared with in-
creasing reaction time (Figure 4). These results are in good
agreement with the electron microscopy investigation.
Figure 5 shows N2 adsorption isotherms of MMM(0),
MMM(1), and MMM(2) calcined at 5508C. The isotherm
14990
ꢁ 2011 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
Chem. Eur. J. 2011, 17, 14987 – 14995