Communication
Dalton Transactions
Notes and references
1 S. Iijima, Nature, 1991, 354, 56.
2 J. T. Hu, T. W. Odom and C. M. Lieber, Acc. Chem. Res.,
1999, 32, 435.
3 Y. Xia, P. Yang, Y. Sun, Y. Wu, B. Mayers, B. Gates, Y. Yin,
F. Kim and H. Yan, Adv. Mater., 2003, 15, 353.
4 J. Zimmerman, R. Parameswaran and B. Z. Tian, Biomater.
Sci., 2014, 2, 619.
5 Z. L. Wang, ACS Nano, 2008, 2, 1987.
Fig. 4 (A) Temperature dependence of magnetization curves and (B)
6 F. S. Kim, G. Ren and S. A. Jenekhe, Chem. Mater., 2010, 23,
682.
hysteresis loops of Fe3O4 nanobelts.
nence values (Mr) are 287.2 Oe and 15.6 emu g−1, respectively,
while the coercivity and remanence values are not obvious at
300 K (Fig. 4B and S4†). The magnetic saturation value at
7 T. Zhai, L. Li, X. Wang, X. Fang, Y. Bando and D. Golberg,
Adv. Funct. Mater., 2010, 20, 4233.
8 T. Zhai, L. Li, Y. Ma, M. Liao, X. Wang, X. Fang, J. Yao,
Y. Bando and D. Golberg, Chem. Soc. Rev., 2011, 40, 2986.
9 N. W. S. Kam, Z. Liu and H. Dai, J. Am. Chem. Soc., 2005,
127, 12492.
10 Y. Lei, Q. Liao, H. Fu and J. Yao, J. Am. Chem. Soc., 2010,
132, 1742.
11 A. Fert and L. Piraux, J. Magn. Magn. Mater., 1999, 200, 338.
12 J. Dorantes-Dávila and G. M. Pastor, Phys. Rev. Lett., 1998,
81, 208.
13 P. Gambardella, A. Dallmeyer, K. Maiti, M. C. Malagoli,
W. Eberhardt, K. Kern and C. Carbone, Nature, 2002, 416,
301.
14 J. R. Morber, Y. Ding, M. S. Haluska, Y. Li, J. P. Liu,
Z. L. Wang and R. L. Snyder, J. Phys. Chem. B, 2006, 110,
21672.
15 S. A. Wolf, D. D. Awschalom, R. A. Buhrman,
J. M. Daughton, S. von Molnár, M. L. Roukes,
A. Y. Chtchelkanova and D. M. Treger, Science, 2001, 294,
1488.
16 R. S. Friedman, M. C. McAlpine, D. S. Ricketts, D. Ham
and C. M. Lieber, Nature, 2005, 434, 1085.
17 Z. M. Liao, Y. D. Li, J. Xu, J. M. Zhang, K. Xia and D. P. Yu,
Nano Lett., 2006, 6, 1087.
300 K is as high as 53 emu g−1
.
As the magnetic anisotropy energy of the nanoparticles de-
posited on certain surfaces can be tuned by the modification
of the size, shape and coupling with the substrate, the syn-
thesis of magnetic nanoparticles with uniform size and con-
trolled shape is tremendously attractive for basic investigations
as well as for miniaturized data storage applications. For nan-
ometer-sized magnetite, shape magnetic anisotropy, depen-
dent on the shape anisotropy and the saturation
magnetization, is believed to be the dominant form of mag-
netic anisotropy. Due to the high magnetic saturation value
(53 emu g−1 at 300 K) and the elongated shape, the as-
obtained Fe3O4 nanobelts exhibit higher anisotropy. The an-
isotropy constant (K) of superparamagnetic nanoparticles can
be calculated from the TB using the equation: K = 25kBTB/V,
where kB is Boltzmann’s constant and V is the volume of a
single nanoparticle.40 For a Fe3O4 nanobelt with a length of
100 nm, the calculated magnetic anisotropy constant is as
high as 6.6 × 104 erg cm−3. Such a value was much higher than
that (5.2 × 103 erg cm−3) of spherical Fe3O4 particles (mean
size: 300 nm) obtained via a similar protocol.20
18 X. Kou, X. Fan, R. K. Dumas, Q. Lu, Y. Zhang, H. Zhu,
X. Zhang, K. Liu and J. Q. Xiao, Adv. Mater., 2011, 23, 1393.
19 Z. Z. Sun and J. Schliemann, Phys. Rev. Lett., 2010, 104,
037206.
20 X. H. Li, D. H. Zhang and J. S. Chen, J. Am. Chem. Soc.,
2006, 128, 8382.
21 L. C. Palmer and S. I. Stupp, Acc. Chem. Res., 2008, 41,
1674.
22 C. Wang, Y. Hou, J. Kim and S. Sun, Angew. Chem., Int. Ed.,
2007, 46, 6333.
Conclusions
We have successfully prepared amphiphilic superparamagnetic
Fe3O4 nanobelts via a novel chemical “top-down” method.
This synthetic approach, using the exfoliated layered material
FeOCl as a precursor, is facile and easy to scale up for large-
quantity application. The as-obtained product, which exhibits
nearly uniform width, superparamagnetic properties, obvious
magnetic anisotropy and excellent dispersibility and redisper-
sibility in most of the common solvents, could be readily used
in various fields such as biomedicine and nanoelectronics.
23 M. Kwiat, S. Cohen, A. Pevzner and F. Patolsky, Nano Today,
2013, 8, 677.
24 B. Mayers and Y. Xia, J. Mater. Chem., 2002, 12, 1875.
25 D. Ung, Y. Soumare, N. Chakroune, G. Viau, M. J. Vaulay,
V. Richard and F. Fiévet, Chem. Mater., 2007, 19, 2084.
Acknowledgements
This work was financially supported by the National Basic 26 L. Bao, W. L. Low, J. Jiang and J. Y. Ying, J. Mater. Chem.,
Research Program of China (2013CB934102, 2011CB808703) 2012, 22, 7117.
and the National Natural Science Foundation of China 27 A. K. Ganguli and T. Ahmad, J. Nanosci. Nanotechnol., 2007,
(21331004, 21301116).
7, 2029.
16176 | Dalton Trans., 2014, 43, 16173–16177
This journal is © The Royal Society of Chemistry 2014