Abstract. This study aimed to investigate the structural characteristics of iron oxide
nanoparticles (IONPs) prepared in different conditions. IONPs were synthesized as aqueous
magnetic fluids by co-precipitation of ferrous and ferric salts, then analyzed by transmission
electron microscopy (TEM), X-ray diffraction (XRD), and Raman scattering spectroscopy.
Results showed that as-prepared IONPs revealed as a mixture of hematite (α-Fe2O3),
maghemite (γ-Fe2O3), and magnetite (Fe3O4) composition. At 900C of reaction temperature,
IONPs showed a good monodispersity and stability, and sizes range from 9.2 to 12 nm.
The Raman spectra also showed the appearance of moderate laser heating in the hematite
structure. The model of IONPs formation was found with a magnetite nucleus and maghemite
that formed the outer layers after the oxidation process.
6 trang |
Chia sẻ: thanhle95 | Lượt xem: 355 | Lượt tải: 0
Bạn đang xem nội dung tài liệu Structural characteritics of iron oxide nanoparticles synthesized by co-precipitation method in different conditions, để tải tài liệu về máy bạn click vào nút DOWNLOAD ở trên
100
HNUE JOURNAL OF SCIENCE DOI: 10.18173/2354-1059.2018-0034
Natural Sciences 2018, Volume 63, Issue 6, pp. 100-105
This paper is available online at
STRUCTURAL CHARACTERITICS OF IRON OXIDE NANOPARTICLES
SYNTHESIZED BY CO-PRECIPITATION METHOD IN DIFFERENT CONDITIONS
Nguyen Thi Luyen
1
, Tran Quang Huy
2,3
and Pham Van Vinh
4
1
Faculty of Physics and Technology, Thai Nguyen University of Science
2
National Institute of Hygiene and Epidemiology,
3
Hung Yen University of Technology and Education
4
Faculty of Physics,
Hanoi National University of Education
Abstract. This study aimed to investigate the structural characteristics of iron oxide
nanoparticles (IONPs) prepared in different conditions. IONPs were synthesized as aqueous
magnetic fluids by co-precipitation of ferrous and ferric salts, then analyzed by transmission
electron microscopy (TEM), X-ray diffraction (XRD), and Raman scattering spectroscopy.
Results showed that as-prepared IONPs revealed as a mixture of hematite (α-Fe2O3),
maghemite (γ-Fe2O3), and magnetite (Fe3O4) composition. At 90
0
C of reaction temperature,
IONPs showed a good monodispersity and stability, and sizes range from 9.2 to 12 nm.
The Raman spectra also showed the appearance of moderate laser heating in the hematite
structure. The model of IONPs formation was found with a magnetite nucleus and maghemite
that formed the outer layers after the oxidation process.
Keywords: Iron oxide nanoparticles, IONPs, co-precipitation, Raman spectra.
1. Introduction
Iron oxide nanoparticles (IONPs) have been widely studied for different applications in the
fields of biomedicine [1, 2], and water treatment [3-5]. IONPs can be effectively prepared by
several methods, in which the co-precipitation method of ferric and ferrous salts has been
popularly used. Interestingly, IONPs exhibit super paramagnetic behavior with sizes of less than
35 nm [6, 7]. Magnetite (Fe3O4) nanoparticles have been proved with many unique magnetic
properties, such as super paramagnetic, low Curie temperature, and high magnetic susceptibility [1, 6],
so they can be applied for various purposes. However, the broad size distribution of IONPs can
result in limitations for further applications. Among four different crystalline polymorphs of
Fe2O3 including γ-Fe2O3, β-Fe2O3, ε-Fe2O3 and α-Fe2O3, the structure of γ-Fe2O3 and α-Fe2O3
phases has been considered rather than the rest [8-10]. γ-Fe2O3, a ferromagnetic material exhibits
the cubic spinel structure at room temperature with a Curie temperature (TC) of 928 K. By contrast,
α-Fe2O3 crystallizes in the corundum structure reveals as the most thermodynamically stable phase.
It is weakly ferromagnetic at room temperature due to the Dzyaloshinsky-Moriya mechanism
and anti-ferromagnetic below 263 K [11-14]. At elevated temperatures of more than 950 K,
α-Fe2O3 shows paramagnetic behavior [15]. Moreover, there are some models available to explain
Received May 23, 2018. Revised August 13, 2018. Accepted August 20, 2018.
Contact Nguyen Thi Luyen, Email: luyennt@tnus.edu.vn.com.
Structural characteristics of iron oxide nanoparticles synthesized by co-precipitation method
101
the formation of IONPs. For examples, Sousa [16] and Wang [17] also have suggested models
with a maghemite nucleus and magnetite forming the outer layers after oxidation. Chroupa et al. [18]
have used Raman confocal multispectral imaging to investigate the chemical and structural
properties of ferrite-based nanoparticles, precursors for magnetic drug targeting, the results
affirmed that oxidized nanoparticles have partly conversed of magnetite into maghemite, and a
model of IONPs formation is also suggested by a magnetite nucleus and maghemite layers. In fact,
the molecular composition of IONPs can vary considerably, depending on experimental
conditions. Through a well-known magnetite oxidation, antiferromagnetic hematite (α-Fe2O3) can
be found [19, 20] or reveals as an amorphous non-stoichiometric oxyhydroxide [FeOx(OH)3-2x, x < 1]
and Fe(OH)3 in magnetite and maghemite nanoparticles [16], resulting in the changes of IONPs
formation.
Furthermore, the structural characteristics of IONPs synthesized in different conditions could
be influential to the monodispersity and stability in the solution as well as magnetic properties
leading to advantage or limitations in various applications [18].
In this work, three methods of TEM, XRD and Raman analyses were employed to investigate
the structural characteristics of IONPs synthesized by the co-precipitation method in different
conditions, particularly, under the systematic changes of reaction temperature, and precursors.
The results would be expected to give supplementary information related to the morphology, size,
crystallinity and the magnetic behavior of Fe3O4, γ-Fe2O3 and α-Fe2O3 nanoparticles synthesized.
2. Content
2.1. Experiments
2.1.1. Materials
Ferric chloride (FeCl3.6H2O), ferrous chloride (FeCl2.4H2O), and ammonia solution
(NH4OH), were purchased from Sigma Aldrich, Merck Chemical Company. Deionized water was
used to prepare all solutions.
2.1.2. Preparation of iron oxide nanoparticles
IONPs were prepared by the co-precipitation of ferric and ferrous ions in deionized water. A
series of two samples was prepared by changing the reaction temperature from 30
o
C to 90
o
C
(denoted by F1 and F5) and concentrations of NH4OH from 0.1 M to 0.23 M (denoted by F5 and F9).
Firstly, by changing the reaction temperature, a mixture of 0.6 g of FeCl2.4H2O and 1.6 g of
FeCl3.6H2O were dissolved in 25 mL of deionized water with the range of temperatures changed
from 30, 45, 60, and 75 to 90
o
C. Then, 5 mL of NH4OH was added drop wise to the mixture with
vigorous stirring. After that, the solution was vigorously stirred for another 30 min. Finally, the
resultant synthesized IONPs were centrifuged and washed with deionized water for several times.
To change concentrations of NH4OH, the reaction temperature was fixed at 75
o
C.
2.1.3. Characterization
Surface morphology, size and dispersion of IONPs were characterized by transmission
electron microscopy (TEM) (JEM 1010, JEOL), operated at 80 kV. Structure of IONPs were
investigated by a D2 X-ray diffractometer equipped with a Cu Kα tube and a Ni filter (λ = 1.542 Ao).
Raman spectra of these samples were recorded by using a high-resolution confocal Raman
microscope (Horiba, LabRam HR) and a 538.14 nm Ar laser source, at the room temperature
under the same experimental condition (18 mW, 20x microscopy objective) with acquisition time
of 10 s.
Nguyen Thi Luyen, Tran Quang Huy and Pham Van Vinh
102
2.2. Results and discussions
2.2.1. Morphology of IONPs
TEM images of IONPs prepared at different temperatures (60
o
C and 90
o
C), for 30 min, are
given in Figure 1. There was no different in size and dispersity of IONPs at the time point of
synthesis and after three months. It can be observed that they are all sphere-like structures. IONPs
prepared at 60
o
C, exhibit serious agglomeration (Figure 1a), while the IONPs prepared at 90
o
C
show a good dispersion (Figure 1b). A histogram of their size distribution has been obtained by
the particle size measurement at different reaction temperatures, which are shown in Figure 1c,
and 1d, respectively. TEM images of IONPs samples at 60
o
C and 90
o
C revealed that the average
particle sizes are about 9.2 nm and 12 nm, respectively, with narrow size distributions. The size of
IONPs increases with the increase of reaction temperature in good dispersion.
Figure 1. TEM images of IONPs obtained at different temperatures: (a) 60
o
C; (b) 90
o
C
and (c), (d) histograms of IONPs size distribution, respectively
2.2.2. XRD patterns and Raman spectra of IONPs
In this study, XRD was performed with IONPs synthesized at different temperatures and
concentrations of NH4OH to investigate the change in crystal structures (Figure 2). Obviously, the
diffraction peaks are indexed by cubic structure of γ-Fe2O3 phase, meet the reference data for
cubic close packed γ-Fe2O3 phase (JCPDS card 39-1356). Both the magnetite and maghemite
phases have the same spinel structure as well as very similar lattice parameters. As seen at 2 theta,
all characteristic peaks are found at 30.58
o
, 36.03
o
, 43.66
o
, 54
o
, 57.55
o
and 63.10
o
, corresponding
to the lattice planes of (220), (311), (400), (422), (511) and (440) of either γ-Fe2O3 phase or Fe3O4
cubic structure. No specific peaks are observed in the samples for any impurities, so it also reveals
Structural characteristics of iron oxide nanoparticles synthesized by co-precipitation method
103
a high phase purity of γ-Fe2O3 or Fe3O4. According to Debye – Scherrer equation, the average
crystallite sizes of two samples at 60
o
C (F3) and 90
o
C (F5) are calculated to be 9.5 and 11.2 nm,
respectively [21].
Figure 2. X-ray power diffraction patterns of IONPs prepared with (a) different temperature
ranging from 30
o
C to 90
o
C (F1-F5); and (b) different concentration of NH4OH
from 0.1 to 0.23 M (F5-F9)
As discussed in the XRD patterns, we found that IONPs still contain a dominant fraction of
magnetite. A model is suggested with a magnetite nucleus, since the magnetite can be preserved
from oxidation only in the inner layers of each nanoparticle. Similar to iron oxidation films,
nanoparticles consist of an inner Fe3O4 and an outer, passive layer of Fe2O3.
Figure 3. Raman spectra of IONPs prepared with (a) different reaction temperature from 30
o
C
to 90
o
C (F1-F5); and (b) different concentrations of NH4OH from 0.1 to 0.23 M (F5-F9)
Raman spectroscopy was used to distinguish the γ-Fe2O3, α-Fe2O3 and Fe3O4. Figure 3 (a, b)
shows the Raman spectrum of two samples series with different reaction temperatures and
concentrations of NH4OH, respectively. The peaks with strong intensity are at about 383 cm
-1
, 582 cm
-1
and 806 cm
-1
,
corresponding to γ-Fe2O3 nanoparticles. The sharp and intense peak at around 806 cm
-1
,
which characteristic of magnetite, can be assigned to A1g vibrational mode of magnetite [18, 22, 23].
In fact, it is not easy to see the difference in crystal structures of IONPs from XRD patterns, for
example, Fe3O4 and γ-Fe2O3 nanoparticles have some diffraction peaks overlapped, so Raman
spectroscopy becomes an advantageous to differ these structures.
Nguyen Thi Luyen, Tran Quang Huy and Pham Van Vinh
104
Figure 4. Spectral changes in the 100 - 900 cm
-1
region for IONPs (F8 sample)
Raman spectra fitted with Lorentz function
Table 1. Raman frequencies (cm
-1
) of as-prepared IONPs
Bulk
hematite
Bulk
magnetite
Bulk
maghemite
Nanophase
in this study
Assignment in the
spectra nanoparticles
s 703 s 806 Maghemite
s 662
w 610
m 411 vw 528
vw 508
vw 456
s 502
s 582
s 484
Maghemite
hematite
w 303 s 330 s 383 Maghemite
ss 292
vw 247
ss 225
w 194 ss 212
ss 275
Hematite
Hematite
The peaks at 383 cm
-1
and 582 cm
-1
can be attributed to T2g vibrational modes of magnetite.
Generally, upon laser-stimulated, hematite structure was formed from pre-initialized oxidation
sites. The remaining peaks with very strong intensity at 212 cm
-1
, 275 cm
-1
and strong intensity at
484 cm
-1
, corresponding to α-Fe2O3 nanoparticles, can be assigned to A1g, E1g and A1g vibrational
modes of hematite [18, 24]. There is no significant Raman peaks assignable to iron oxyhydroxide
goethite (α-FeOOH) or lepidocrocite (γ-FeOOH) [18, 20, 24].
Through the information of structural characteristics, it is clear that IONPs formed by a
magnetite nucleus and outer layers of maghemite after the oxidation process, and it can be
influential to their stability, monodispersity, and also magnetic properties. In this study, the
magnetic characteristics of as-synthesized IONPs have not investigated yet, but it should be done
according to the structural changes of IONPs synthesized in different conditions, and also the
purpose of particular applications.
Structural characteristics of iron oxide nanoparticles synthesized by co-precipitation method
105
3. Conclusion
In summary, iron oxide nanoparticles have been successfully synthesized using the co-
precipitation method in different conditions, and their structural characteristics are investigated.
IONPs are found with good monodispersity, and stability at the reaction temperature of 90
o
C, and
their sizes are in the range of 9.2 to 12 nm. As-synthesized IONPs have a mixed magnetite-
maghemite structures under XRD investigation, while Raman spectroscopy reveals the presence
of hematite structure in the samples. The model of IONPs formation is also confirmed with a
magnetite nucleus and maghemite layers. Together with the information of structural
characteristics of IONPs investigated by Raman confocal multispectral imaging, the results would
be helpful for various applications, particularly in drug targeting and delivery.
Acknowledgements: This research was supported by the bilateral project between Italy and
Vietnam, coded NĐT.05.ITA/15.
REFERENCES
[1] Y. L. Chueh, M. W. Lai, J. Q. Liang, L. J. Chou and Z. L. Wang, 2006. Adv. Funct. Mater.
16 2243.
[2] P. P. Yang, S. L. Gai and J. Lin, 2012. Chem. Soc. Rev. 413679.
[3] T. Q. Huy, P. V. Chung, N. T. Thuy, C. Blanco-Andujar and N. T. K Thanh, 2014. Faraday
Discuss. 175, 73.
[4] D. H. K. Reddy and S. M Lee, 2014. Colloid Surf. A-Physicochem. Eng. Asp. 454, 96.
[5] F. Ma, B. Zhao and J. Diao, 2016. Water Sci. Technol. 74, 1335.
[6] R. E. Rosensweig, 1997. Ferrohydrodynamics, Dover, New York.
[7] C. P. Bean and J. D. Livingstone, 1959. J. Appl. Phys. 40, 120.
[8] R. M. Cornell and U. Schwertmann, 2003. The Iron Oxides: Structure, Properties,
Reactions, Occurences and Uses, Second Edition. Wiley-VCH, Weinheim, Germany.
[9] R. Zboril, M. Mashlan and D. Petridis, 2002. Chem. Mater. 14, 969.
[10] J. Tucek, R. Zboril, A. Namai and S. I. Ohkoshi, 2010. Chem. Mater. 22, 6483.
[11] F. J. Morin, 1950. Phys. Rev.78, 819.
[12] J. O. Artman, J. C. Murphy and S. Foner, 1965. Phys. Rev. 138 A912.
[13] T. Moriya, 1960. Phys. Rev. 120, 91.
[14] I. Dzyaloshinsky, 1958. J. Phys. Chem. Solids 4, 241.
[15] L. Neel, 1949. Ann. Phys. 4, 249.
[16] M. H. Sousa, F. A. Tourinho and J. C. Rubim, 2000. J. RamanSpectrosc, 31, 185.
[17] Z. Wang and S. K. Saxena, 2002. Solid State Commun. 123, 195.
[18] I. Chourpa, L. D. Eyrolles, L. N. Okassa, J. F.Fouquenet, S. C. Jonathan, M. Souce, H.
Marchais and P. Dubois, 2005. Ro. Soc. Chem. 130, 1395.
[19] J. Tang, M. Myers, K. A. Bosnick and L. E. Brus, 2003. J. Phys. Chem. B 107. 7501.
[20] A. P. Kozlova, S. Sugiyama, A. I. Kozlov, K. Asakura and Y. Iwasawa, 1998. J. Catal. 176, 426.
[21] J. Hu, X. Hu, A. Chen, S. Zhao, 2014. J. Alloys Compounds 603, 1.
[22] D. L. A. De Faria, S. Venancio Silva and M.T. DeOliveira, 2007. J. Raman Spectrosc. 28, 873.
[23] I. Chamritski and G. Burns, 2005. J. Phys. Chem. B 109, 4965.
[24] D. L. A. de Faria, S. V. Silva and M. T. Oliveira, 1997. J. RamanSpectrosc. 28, 873.