6
Journal of the American Ceramic Society—Lee et al.
Fe(acac)3 (100 g) and 1-hexadecanol (409 g) in 2 L glass bea-
ker at room temperature, and (b) the set-up for thermal
decomposition reaction (300°C).
Fig. S2. Photographs of (a) the produced nanocrystals of
20.3 g and attraction of (b) the powder and (c) nanoparticles
dispersed in toluene by external magnetic field.
Fig. S3. Gas chromatogram of the solvent (1-hexadecanol)
from Sigma-Aldrich without further purification. The prod-
ucts are as follows: (1) 16-hydroxyhexadecanoic acid, and (3)
1-hexadecanol.
Fig. S4. TEM images and particle size distribution his-
tograms of Fe3O4 nanocrystals with an average size of (a)
7.8 ꢀ 0.6 nm, (b) 6.5 ꢀ 0.4 nm, and (c) 5.9 ꢀ 0.2 nm.
Fig. S5. SAED pattern of the 7.8 nm-sized Fe3O4
nanocrystals.
Fig. S6. Rietveld refinement patterns of the 7.8 nm-sized
Fe3O4 nanocrystals using X-ray powder diffraction. Black
solid line represent the observed pattern, and the red dot
mark(o) is calculated result. The difference plot (blue) is
shown at bottom. Tick marks indicate the reflection posi-
tions, which are identified by Rietveld analysis. The pub-
lished crystal structure of Fe3O4 was employed as a starting
structural model (ICSD # 6534).
Table S1. Refined crystal structural parameters of Fe3O4
nanocrystals obtained from the Rietveld refinement using
X-ray powder diffraction data at room temperature. The sym-
bols, O and Biso, represent the occupation and isotropic ther-
mal parameters, respectively. The numbers in parentheses are
the estimated standard deviations of the last significant figure.
Fig. 7. Magnetic hysteresis loops of (a) Fe3O4 nanocrystals
(average size of 7.8 ꢀ 0.6 nm), and porous Fe3O4 nanocrystals of
average size of (b) 25 ꢀ 2.7 and (c) 36 ꢀ 3.2 nm.
low remanence values of about 4.78, 5.97, and 10.5 emu/g.
Generally, the saturation magnetization (MS) is expected to
increase with an increasing particle size.22,25,26 However, the
MS value of porous Fe3O4 nanocrystals decreased with the
increasing particle size of the nanocrystals. The MS values of
porous Fe3O4 nanocrystals (25 ꢀ 2.7 and 36 ꢀ 3.2 nm sam-
ples) roughly accounts for 51% (47.22 emu/g), and 27%
(25.25 emu/g) of the corresponding bulk value (92 emu/g).
This unusual behavior seems to be attributable to the porous
nature of our Fe3O4 nanocrystals. The MS values were com-
monly reported to be smaller (by 20%–25%) for hollow
nanoparticles than those for the bulk.15 Ongoing work will
involve an investigation of the detailed formation mecha-
nisms and magnetic properties of porous Fe3O4 nanocrystals.
References
1M. V. Rdddy, G. V. Subba Rao, and B. V. R. Chowdari, “Metal Oxides
and Oxysalts as Anode Materials For Li Ion Batteries,” Chem. Rev., 113 [3]
5364–457 (2013).
2Y.-W. Jun, J.-S. Choi, and J. Cheon, “Shape Control of Semiconductor
and Metal Oxide Nanocrystals Through Nonhydrolytic Colloidal Routes,”
Angew. Chem. Int. Ed., 45 [21] 3414–39 (2006).
3A. Kudo and Y. Miseki, “Heterogeneous Photocatalyst Materials for
Water Splitting,” Chem. Soc. Rev., 38 [1] 253–78 (2009).
IV. Conclusion
4S. Laurent, D. Forge, M. Port, A. Roch, C. Robic, et al., “Magnetic Iron
Oxide Nanoparticles: Synthesis, Stabilization, Vectorization, Physicochemical
Characterizations, and Biological Applications,” Chem. Rev., 108 [6] 2064–110
(2008).
We reported a facile process for the synthesis of Fe3O4
nanocrystals via the thermal decomposition of Fe(acac)3 in
1-hexadecanol. Formation mechanisms were elucidated on
the basis of GC-MS analysis, which enabled large-scale
nanocrystal preparation. The resulting nanocrystals had a
spherical shape with average diameters of 7.8 ꢀ 0.6,
6.5 ꢀ 0.4, and 5.9 ꢀ 0.2 nm when prepared at 300°C, 270°C,
and 250°C, respectively. This synthetic method had a high
yield and good reproducibility. Furthermore, to demonstrate
economical application, porous Fe3O4 nanocrystals were pre-
pared using recycled solvent, which was recovered from pre-
vious processes. The resulting Fe3O4 nanocrystals with
porous structures had larger average sizes of 25 ꢀ 2.7 and
36 ꢀ 3.2 nm than those obtained from the initial process.
These results indicate a promising durable route for the
large-scale preparation of nanocrystals with controlled sizes
and morphologies.
5T. J. Daou, G. Pourroy, S. Begin-Colin, J. M. Greneche, C. Ulhaq-Bouil-
let, et al., “Hydrothermal Synthesis of Monodisperse Magnetite Nanoparti-
cles,” Chem. Mater., 18 [18] 4399–404 (2006).
6N. Pinna, G. Garnweitner, M. Antonietti, and M. A. Niederberger, “Gen-
eral Nonaqueous Route to Binary Metal Oxide Nanocrystals Involving a C-C
Bond Cleavage,” J. Am. Chem. Soc., 127 [15] 5608–12 (2005).
7M. Barroso, A. J. Cowan, S. R. Pendlebury, M. Gratzel, D. R. Klung, and
J. R. Durrant, “The Role of Cobalt Phosphate in Enhancing the Photocat-
alytic Activity of a-Fe2O3 Toward Water Oxidation,” J. Am. Chem. Soc., 133
[38] 14868–71 (2011).
8U. Sobocan, G. Lee, H.-W. Kang, H. J. Kim, Z. Jaglicic, and J. Dolinsek,
“The Nature of Magnetic State of Small Fe3O4 Nanoparticles,” J. Analytical.
Sci. Technol, 2 [Suppl. A] A8–14 (2011).
9S. Lee, H.-W. Kang, M. Kwak, Y.-J. Lee, G. Lee, et al., “Indentification
of Spinel Iron Oxide Nanoparticles by 57NMR,” J. Analytical. Sci. Technol, 2
[Suppl. A] A81–7 (2011).
10H. M. Rietveld, “Line Profiles of Neutron Powder-Diffraction Peaks for
Structure Refinement,” Acta Crystallogr, 22 [1] 151–2 (1967).
11AXS Bruker, TOPAS V2.0: General Profile and Structure Analysis Soft-
ware for Powder Diffraction Data; User Manual. Bruker AXS, Karlsruhe, Ger-
many, 2000.
Acknowledgments
12A. Kern, A. A. Coelho, and R. W. Cheary, “Convolution Based Profile
Fitting”; pp. 17–50 Chapter 2 in Diffraction Analysis of the Microstructure of
Materials, Edited by E. J. Mittemeijer and P. Scardi. Springer, Berlin, Ger-
many, 2004.
We acknowledge KBSI grants (no. C36957) for financial support of this
project. This work was supported by Small and Medium Business Administra-
tion (S2060417) and the Basic Science Research Program through the
National Research Foundation of Korea (NRF) funded by the Ministry of
Science, ICT & Future Planning (NRF-2015R1C1A1A02037373, NRF-
2014R1A6B1A01048313, and NRF-2013R1A2A2A01067144).
13R. W. Cheary and A. Coelho, “A Fundamental Parameter Approach of
X-ray Line-Profile Fitting,” J. Appl. Cryst, 25 [2] 109–21 (1992).
14J. Park, K. An, Y. Hwang, J.-G. Park, H.-J. Noh, et al., “Ultra-Large-
Scale Syntheses of Monodisperse Nanocrystals,” Nat. Mater., 3 [12] 891–5
(2004).
Supporting Information
15K. M. Nam, J. H. Shim, H. Ki, S.-I. Choi, G. Lee, et al., “Single-Crys-
talline Hollow Face-Centered-Cubic Nanoparticles From Solid Face-Cen-
tered-Cubic Oxide Nanoparticles,” Angew. Chem. Int. Ed., 47 [49] 9504–8
(2008).
Additional Supporting Information may be found in the
online version of this article:
16J. H. Shim, K. M. Nam, W. S. Seo, H. Song, and J. T. Park, “The Role
of Water for the Phase-Selective Preparation of Hexagonal and Cubic Cobalt
Oxide Nanoparticles,” Chem. Asian J., 6 [6] 1575–81 (2012).
Fig. S1. Photographs of experimental procedure for large-
scale synthesis of the Fe3O4 nanocrystals. (a) the mixture of