Cobalt Flowerlike Architectures by a Facile Hydrothermal Route
netic field of 20 kOe was applied. As shown in Figure 8,
the coercivities at 5 K and 295 K are 371 Oe and 197 Oe,
Experimental Section
All reagents used were commercial products of analytical pure
grade, and they were used without further purification. In a typical
procedure, CoCl2·6H2O (0.238 g, 1 mmol), dodecyl benzenesulfo-
nate (SDBS) (0.116 g, 0.5 mmol), and NaOH (1.6 g, 40 mmol) were
first dissolved in distilled water (40 mL), and the solution was con-
stantly stirred for 15 min at room temperature. After addition of
NaH2PO2·H2O (1.7 g, 16 mmol), the solution was constantly
stirred for another 15 min. Then the solution was transferred into
a 50 mL Teflon-lined stainless steel autoclave. The autoclave was
sealed and maintained at 180 °C for 6–24 h and then cooled to
room temperature naturally. The product was filtered off, washed
with distilled water and ethanol for several times, finally dried in a
vacuum oven at 60 °C for 4 h. Control experiments were carried
out by adjusting the reaction temperature (100–180 °C) and the
amount of NaOH (1–5 ), while keeping other reaction parameters
unchanged.
respectively. Relative to bulk cobalt (a few tens of Oe[16]
)
and cobalt hollow spheres (66 Oe, 300 K[21]), the coercivity
at room temperature is enhanced, which can probably be
attributed to the high shape anisotropy of the hexagonal
sheets on the flowerlike architectures. However, although
their morphologies are similar, the coercivity (371 Oe) of
the present product at 5 K is much lower than that of the
reported spheres (590 Oe, 5 K),[24] which might be because
of the larger size of the present product (Table 1) and the
higher reaction temperature. The saturation magnetization
at 295 K of the flowerlike structures is 150.4 emu/g, which
is slightly lower than that of its bulk counterpart (168 emu/
g).[14] The result is consistent with other previous reports,
which was ascribed to the reduction of the saturation mag-
netization because of the existence of impurities,[31] surface
antiferromagnetic oxidation,[31] and surface spin disor-
der.[32] In the present case, all of these factors may be re-
sponsible for the reduction of the saturation magnetization.
The phases of all products were identified with a Rigaku D/max
2500pc X-ray diffractometer (XRD) with Cu-Kα radiation (λ =
1.54156 Å) at a scan rate of 0.04 °s–1. The morphology was investi-
gated with a Shimadzu SSX-550 scanning electron microscope
equipped with an EDS system operated at an acceleration voltage
of 15.0 kV. Transmission electron microscopy (TEM) was carried
with a TECNAI 20 instrument having an emission voltage of
200 kV. Magnetic hysteresis loops were measured by using a
MPMS-7 superconducting quantum interference device (SQUID)
magnetometer at fields up to 20 kOe.
Supporting Information (see footnote on the first page of this arti-
cle): SEM images of the products at 140 °C and 160 °C; SEM im-
age of the product at 180 °C in the absence of SDBS; SEM images
of the products at 180 °C with SDS and CTAB.
Acknowledgments
This work has been supported by the National Natural Science
Foundation of China under Grant No. 50331030.
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Figure 8. Magnetic hysteresis loops at 5 K (solid circles) and 295 K
(open circles) of the product obtained at 180 °C after reaction for
24 h. The inset shows the low-field part of the hysteresis loops.
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Mesoscale formation of cobalt flowerlike hierarchical
architectures self-assembled by hexagonal nanosheets has
been fabricated in a controlled manner by a hydrothermal
process in the presence of SDBS. It has been found that the
surfactant SDBS, the reaction temperature, and the concen-
tration of NaOH are key parameters for the fabrication of
the complex 3D structures. The growth mechanism for the
formation of the flowerlike architectures has been eluci-
dated: the intermediate product Co(OH)2 plays a critical
role in the generation of sheet-shaped cobalt, and then the
cobalt nanoplates assemble into flowers. The products exhi-
bit ferromagnetic behavior. Such a simple and mild syn-
thetic approach can be extended to the controlled synthesis
of 3D hierarchical architectures of other materials.
Eur. J. Inorg. Chem. 2008, 2733–2738
© 2008 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
www.eurjic.org
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