a new cofe2o4cr2o3sio2 fluorescent magnetic nanocomposite
TRANSCRIPT
PAPER www.rsc.org/nanoscale | Nanoscale
Dow
nloa
ded
on 1
5 O
ctob
er 2
010
Publ
ishe
d on
10
Sept
embe
r 20
10 o
n ht
tp://
pubs
.rsc
.org
| do
i:10.
1039
/C0N
R00
281J
View Online
A new CoFe2O4–Cr2O3–SiO2 fluorescent magnetic nanocomposite
Chandan Borgohain,ab Kula Kamal Senapati,ab Debabrata Mishra,b Kanak Ch. Sarmac and Prodeep Phukan*a
Received 27th April 2010, Accepted 2nd July 2010
DOI: 10.1039/c0nr00281j
A combined sonochemical co-precipitaion method has been developed for the synthesis of a CoFe2O4–
Cr2O3–SiO2 magnetic nanocomposite. The synthesis involved the pre-synthesis of CoFe2O4–Cr2O3
nanoparticles, which were subsequently coated with SiO2 by treatment with tetraethyl orthosilicate. It
was observed that the as-prepared CoFe2O4–Cr2O3–SiO2 nanocomposite exhibits photoluminescence
properties without the addition of any external fluorescent marker. The fluorescent magnetic
nanoparticles (FMNPs) had a typical diameter of 30� 5 nm and a saturation magnetization of 5.1 emu
g-1 at room temperature. This as-prepared nanocomposite was used for staining cultured HeLa cells for
fluorescence imaging.
Introduction
Magnetic nanoparticles have drawn significant attention in
recent years from both a fundamental point of view and for
applications in material science.1–4 Such particles are in high
demand as new nanoscale technologies are beginning to change
the scientific landscape in terms of medical diagnosis, treatment
and prevention.5–7 Cobalt ferrite (CoFe2O4) is one of the most
extensively studied ferrites and has been exploited for its
potential utilization as an active component for high-density
magnetic storage, spintronic devices and for the fabrication of
sensors for biomedical applications and hyperthermia.8–10 Soler
et al.11 have shown that CoFe2O4 has high structural stability
and is reliable as a magnetic drug carrier in biological appli-
cations. Chromium oxide (Cr2O3) on the other hand is an
important material since it has a high melting temperature, is
resistance to oxidation and exhibits interesting optical, elec-
trical and magnetic properties.12,13 Magnetically CoFe2O4–
Cr2O3 is a two-phase exchanged coupled system consisting of
a ferromagnet (CoFe2O4) biased by an antiferromagnet (Cr2O3)
and such systems with ferro-antiferromagnetic coupling have
been extensively studied in light of magnetoresistive read-head
applications.14,15
Recently, several types of nanoparticle have been used for
bioanalysis. These include dye-doped nanoparticles,16 quantum
dots (QDs),17 lanthanide (Ln3+) doped nanoparticles,18
magnetic nanoparticles19 and gold nanorods.20 These nano-
particles have their own unique properties and have been
adapted for different applications in the field of bioanalysis.
Compared with conventional organic dyes, luminescent nano-
particles are preferred as probes for bioapplications because of
their photostability and strong luminescence. For instance, QD-
integrated magnetic nanoparticles have been actively studied
due to their excellent optical properties such as having narrow
emission bands, continuous broad-band absorption and a high
aDepartment of Chemistry, Gauhati University, Guwahati, 781014 Assam,India. E-mail: [email protected]; Fax: +91-361-2700311; Tel: +91-361-2570535bIndian Institute of Technology Guwahati, Guwahati, 781039 Assam, IndiacDepartment of Instrumentation and USIC, Gauhati University, Guwahati,781014, Assam, India
2250 | Nanoscale, 2010, 2, 2250–2256
resistance to photobleaching in comparison to organic dyes.
However the separation between the magnetic nanoparticles
and the QDs is controlled using a layer-by-layer (LBL)
approach21 to prevent quenching. Such nanoparticles are
usually large (70–100 nm) affecting their stability. Moreover,
this method uses reagents such as polyelectrolytes which are
expensive.
For many applications such as magnetic recording and tar-
geted drug delivery, particles with a higher magnetic moment and
larger particle size are required. Furthermore it is difficult to
produce non-agglomerated nanocrystals of ferromagnetic
nanoparticles. Often larger particles (�50 nm), just below the
superparamagnetic threshold, are more suitable for applications
such as targeted drug delivery as these parameters may influence
drug loading, drug release, stability, toxicity and biological fate.
Much effort has been made to synthesize cobalt ferrite with well-
defined properties. These include important examples such as
mechanochemical methods,22 sonochemical reactions,23 co-
precipitation,24 micro-emulsion procedures,25 and others.26–32
One of the major disadvantages in most of these techniques is the
lower degree of crystallinity in the resulting material, leading in
turn to significant spin misalignment which reduces the net
magnetic moment of the particle.
In this report we describe a method for the synthesis of
a Cr2O3-doped CoFe2O4 nanoparticles coated with a monolayer
of SiO2. A combined co-precipitation sonochemical technique
has been developed in order to obtain highly crystalline magnetic
nanoparticles of 30� 5 nm particle size. It was observed that this
nanocomposite shows photoluminescence properties without the
extra addition of any fluorescent marker. The use of magnetic
fluid nanoparticles (MFNPs) was tested for bio-imaging human
cervical cancer cells (HeLa). While no studies of such CoFe2O4–
Cr2O3–SiO2 nanoparticles for in vitro and in vivo applications
have been reported so far, such conjugates may been used as
bioprobes in which the fluorescent part may be used as an
effective tool for imaging biological cells while the magnetic part
may be used as a therapeutic agent for performing hyperthermia
treatment. The development of such a MFNP with properties for
bio-imaging and for the transport of pharmaceuticals to specific
sites in the body constitutes a powerful tool for gene/drug
therapy.33
This journal is ª The Royal Society of Chemistry 2010
Dow
nloa
ded
on 1
5 O
ctob
er 2
010
Publ
ishe
d on
10
Sept
embe
r 20
10 o
n ht
tp://
pubs
.rsc
.org
| do
i:10.
1039
/C0N
R00
281J
View Online
Experimental
The synthesis of the CoFe2O4–Cr2O3–SiO2 magnetic nano-
composite was achieved in three successive steps. Initially
uncapped CoFe2O4 was synthesized which was then coated with
Cr2O3. Subsequent treatment of the CoFe2O4–Cr2O3 nano-
particles with trietylorthosilicate produced the CoFe2O4–Cr2O3–
SiO2 magnetic nanocomposite. The procedure is described
below.
Synthesis of CoFe2O4 nanoparticles
Two aqueous solutions of FeCl3 (1.5 g, 9.3 mmol, 50 mL) and
CoCl2$6H2O (1 g, 4.2 mmol, 50 mL) were mixed in a 200 mL flat
bottom flask and placed in an ultrasonic bath. An aqueous KOH
solution (3 M, 25 mL) was added dropwise under an argon
atmosphere with continuous ultrasonic irradiation (frequency 40
kHz at 40 kW). Prior to mixing, all these three solutions were
sonicated for 30 min to remove dissolved oxygen. The tempera-
ture of the sonicator bath was raised up to 60 �C and the mixture
was sonicated for a further 30 min in air. The reaction mixture
was centrifuged (14 000 rpm) at ambient temperature for 15 min.
The mixture was further subjected to successive sonication (30
min) and centrifugation (15 min) five times. The black precipitate
was then separated, washed with copious amounts of distilled
water followed by ethanol and kept overnight in an incubator at
60 �C for ageing. The precipitate was further dried in an oven at
100 �C for one hour and subsequently kept under high vacuum
(10�2 bar) for one hour. Finally, the black particles were placed in
50 mL of dry ethanol and subjected to successive sonication (30
min) and centrifugation (15 min) repeatedly until a brown
solution appeared. The precipitate was separated, dried and used
for further modification.
Synthesis of the CoFe2O4–Cr2O3 nanocomposite
The coating of a layer of Cr2O3 on the surface of CoFe2O4
nanoparticles was achieved by premixing a dispersion of
CoFe2O4 nanoparticles in deionised water with appropriate
molar ratios of Cr(OAc)3$H2O in a round-bottom flask in an
ultrasonic bath. An aqueous solution of NaOH was added to the
mixture in the presence of ultrasonic irradiation (frequency 40
kHz at 40 kW). Prior to mixing, all these four solutions were
degassed by sonication for 30 min. The temperature of the son-
icator bath was raised to 60 �C and the mixture was sonicated for
a further 30 min in air. Brown precipitate formation was
observed during this time. The reaction mixture was centrifuged
(10 000 rpm) at ambient temperature for 15 min. The brown
precipitate was then separated, washed with copious amounts of
distilled water followed by ethanol and kept overnight in an
incubator at 60 �C for ageing. The precipitate was further dried
in an oven at 100 �C for one hour and subsequently kept under
high vacuum (10�2 bar) for one hour. Finally, the particles were
placed in 50 mL of dry ethanol and subjected to successive
sonication (30 min) and centrifugation (15 min) repeatedly until
a brown solution appeared. The precipitate was separated, dried
and held at 1000 �C in a muffle furnace for 10 hours to obtain
a fine black powder. Energy-dispersive X-ray spectroscopy
(EDX) analysis at this point showed excellent agreement between
This journal is ª The Royal Society of Chemistry 2010
expected and observed values of the constituent elements which
therefore confirmed the formation of CoFe2O4–Cr2O3.
Surface modification of CoFe2O4–Cr2O3 nanoparticles
The third synthesis step involves silica coating of the as-prepared
CoFe2O4–Cr2O3 nanoparticle surfaces by the hydrolysis of tet-
raethyl orthosilicate (TEOS).34 The CoFe2O4–Cr2O3 nano-
particles (0.2 g) were dispersed in a mixture of ethanol (20 mL),
water (9 mL) and ammonia (25%, 0.5 mL) under ultrasonication
and then TEOS (0.5 mL) was added to the mixture. After three
hours, the precipitate was isolated by centrifugation, washed
with ethanol and water several times and dried at 80 �C under
vacuum for two hours.
Cell labeling
In the cell-labeling process, the cells were cultured in a 25 cm2
glass culture vial and the culture medium was a mixture of
DMEM (Dulbecco’s modified Eagle’s medium), 10% inactivated
fetal bovine serum, 50 units mL�1 of penicillin, 40 mg mL�1 of
streptomycin, and 0.3 mg mL�1 of L-glutamine. Cells were
cultured at 37 �C in a humidified atmosphere that was supplied
with 5% CO2. When the number of cells reached �105 cells per
vial, the culture medium was removed, and a mixture of 0.2 mL
of nanoparticles in PBS buffer (2 mg mL�1) was added to the
culture vial. After incubation for 20 h at 35 �C in 5% CO2 ,�95%
air incubator, the culture vial was washed 16 times using PBS
buffer and was subjected to transmission electron microscopy
(TEM) and fluorescence imaging.
Cell viability experiments
The antiproliferative assay was carried out using a standard
methylthiazoltetrazolium bromide (MTT) assay. The cells (5 �104 cells in each 100 mL medium well) were plated in 0.07%
DMSO as a control in 96-well plates and were incubated for 24 h.
At the end of the treatments, each well was treated with MTT (10
mL), and after incubation for two hours, the absorption at 570
nm was read with a microplate reader.
Characterization
To investigate the formation of CoFe2O4–Cr2O3 nano-
composites, IR studies and X-ray diffraction patterns were
recorded on a Perkin–Elmer RXI FT-IR spectrometer using KBr
pellets and on a Bruker AXD D8 using Cu Ka radiation (l ¼1.54178 �A). The samples for TEM were prepared by drying an
ethanol dispersion of the particles on a carbon-coated copper
grid. The particles were imaged on a 200 kV, JEOL JEM2100
transmission electron microscope. Quantitative elemental anal-
ysis was carried out with an Oxford energy-dispersive X-ray
spectrometer mounted on the transmission electron microscope.
The magnetic properties of the as-prepared CoFe2O4, CoFe2O4–
Cr2O3 and CoFe2O4–Cr2O3–SiO2 nanoparticles were investi-
gated using a vibrating sample magnetometer (Lakeshore 7410).
UV–visible spectra and fluorescent spectra of the nanoparticles
were recorded using a Varian Cary50 biospectrophotometer and
Edinburgh FSP920 Instruments respectively. Quantum yield
evaluations were made by comparing the integrated intensity of
Nanoscale, 2010, 2, 2250–2256 | 2251
Dow
nloa
ded
on 1
5 O
ctob
er 2
010
Publ
ishe
d on
10
Sept
embe
r 20
10 o
n ht
tp://
pubs
.rsc
.org
| do
i:10.
1039
/C0N
R00
281J
View Online
the luminescence of the sample with a standard solution of
quinine sulphate. The UV–visible absorbance spectrum of the
reference solvent and the sample solution were noted at the
excitation wavelength of 260 nm and 360 nm. Cell labeling
experiments were conducted under fluorescence microscopy
using a Carl Zeiss, LSM 510 meta confocal laser scanning
microscope.
Results and discussion
Structural and morphological analysis
To understand the mechanisms behind the magnetic properties,
we carried out detailed magnetic and microstrucural studies. The
fluorescent properties of the nanoparticles were studied using
a time-resolved steady-state photoluminescence spectrometer.
Pure magnetic nanoparticles however may not be very useful in
practical applications as they are likely to form large aggregates
and their magnetic properties would change or they may undergo
rapid biodegradation when they are exposed to biological
systems. To remove these drawbacks we coated the nanoparticles
with a layer of SiO2.
Fig. 1(a) shows the XRD pattern of the CoFe2O4–Cr2O3
nanocomposite. The diffraction peaks and relative intensities of
the pattern match well with the cubic spinel structure of CoFe2O4
(JCPDS–International center diffraction data, PDF cards 3-864
and 22-1086) and of Cr2O3 (JCPDS–International center
diffraction data, PDF cards 06-0504).
Fig. 1 (a) XRD pattern and (b) FT-IR spectra of the as-prepared
CoFe2O4–Cr2O3 particles.
2252 | Nanoscale, 2010, 2, 2250–2256
The crystallite size (D) of the nanoparticles were determined
using the Scherrer formulae35 on the (311) peak of CoFe2O4 and
was found to be 30 nm. The FT-IR spectra of the material
(Fig. 1b) showed peaks at 611, 938, 1037, 1180, 1338 and 1586
cm�1 corresponding to CoFe2O4 and peaks at 575, 624, 923,
1155, 1528 and 1638 cm�1 corresponding to CoFe2O4–Cr2O3.
The peak obtained at 611 cm�1 in the CoFe2O4 samples is
attributed to the Fe–O or the Co–O bond.36 In the CoFe2O4–
Cr2O3 samples the peak at 575 cm�1 corresponds to the Cr–O
bond.37
The structural composition and crystallinity of the cobalt
ferrite nanoparticles was further examined using TEM. Fig. 2
shows the TEM image of the cobalt–ferrite nanocrystals depos-
ited on a carbon-coated copper grid. A TEM image of the
CoFe2O4–Cr2O3 nanoparticle is shown in Fig. 2a and Fig. 2b
shows the TEM image of the CoFe2O4–Cr2O3–SiO2 nano-
composite. The SAED pattern (Fig. 2d) obtained from TEM
showed CoFe2O4–Cr2O3–SiO2, with the rings corresponding to
reflections from the planes of CoFe2O4, Cr2O3 and SiO2. The
average size of the nanoparticles from the TEM analysis
(Fig. 2a–b) was found to be 30 � 5 nm.
Magnetic properties
It is well known that the magnetic properties of CoFe2O4 depend
on the chemical nature of Co, since Fe3+ species are evenly
distributed in the structure at tetrahedral and octahedral inter-
stices and are antiferromagnetically coupled. Such coupling
cancels the moment contribution from Fe3+ and hence the
moment contribution is solely dependent on Co2+.38 Incorpora-
tion of antiferromagnetic Cr2O3 and SiO2 in the Co–Fe–O matrix
may cause changes in the magnetic properties of the material.
The Magnetisation–Hysteresis (M–H) loop was taken at room
temperature with a maximum applied field of � 2 T. From the
hysteresis loop, both saturation magnetization, coercivity and
retentivity values were extracted.
Fig. 3 shows that the prepared CoFe2O4–Cr2O3–SiO2 particles
are ferromagnetic at room temperature with a saturation
magnetization of 5.1 emu gm�1 and coercivity of 482 Oe. It has
recently been demonstrated by Jordan et al.39 that large coer-
civity magnetic nanoparticles have the ability to self-heat when
irradiated by electromagnetic irradiation. This is known as
magnetic fluid hyperthermia (MFH)40 and can act as a thera-
peutic agent by itself. It can be seen from Table 1 that incorpo-
ration of Cr2O3 and SiO2 into the Co–Fe–O matrix has very little
effect on the coercivity, however the magnetization and the
retentivity decrease rapidly. Therefore by controlling the quan-
tity of Cr2O3 and SiO2 in the Co–Fe–O matrix, magnetic prop-
erties of the nanocomposite can be tailored to suite different
biomedical applications.
Spectral analysis
We have performed room-temperature optical absorption and
photoluminescence to show the optical properties of the nano-
composite compared to its individual component (Cr2O3). Fig. 4
(a–d) shows the UV–visible absorption and fluorescence emis-
sion spectra of the CoFe2O4–Cr2O3–SiO2 particles. The sharp
This journal is ª The Royal Society of Chemistry 2010
Fig. 2 TEM images. (a) TEM image of CoFe2O4–Cr2O3,(b) TEM image
of CoFe2O4–Cr2O3–SiO2 nanocomposite, (c) HRTEM images of
CoFe2O4–Cr2O3–SiO2 nanocomposite and (d) SAED pattern of
CoFe2O4–Cr2O3–SiO2 nanocomposite.
Fig. 3 Hysteresis curves of CoFe2O4, CoFe2O4–Cr2O3 and CoFe2O4–
Cr2O3–SiO2 nanocomposites.
Table 1 Effect of the incorporation of antiferromagnetic Cr2O3 andSiO2 into the Co–Fe–O matrix on its magnetic properties
NanocompositeCoercivity/Oe
Magnetization/mass emu gm�1
Retentivity/emu gm�1
CoFe2O4 539 64.97 17.49CoFe2O4–Cr2O3 529 24.74 6.62CoFe2O4–Cr2O3–SiO2 482 5.10 1.79
This journal is ª The Royal Society of Chemistry 2010
Dow
nloa
ded
on 1
5 O
ctob
er 2
010
Publ
ishe
d on
10
Sept
embe
r 20
10 o
n ht
tp://
pubs
.rsc
.org
| do
i:10.
1039
/C0N
R00
281J
View Online
peak at 200 nm in the UV–visible spectra indicates that the
colloids are well dispersed.
The UV–visible spectra of CoFe2O4–Cr2O3and Cr2O3 showed
absorption bands at around 260 and 360 nm. The bandgap
corresponding to the absorption bands was calculated by plot-
ting (ahn)2 vs. hn (Fig. 4b) using the relationship:41
ahn ¼ const (hn � Eg)n (1)
The value of a is obtained from the equation:42
a ¼ 2:3026
�A
t
�(2)
Where A is the absorption and t is the thickness of the sample.
Fig. 4 (a–b) Absorption spectra of CoFe2O4–Cr2O3–SiO2 at different
concentrations, (c–d) absorbance of nanocomposites in DMEM over
a period of 24 hrs.
Nanoscale, 2010, 2, 2250–2256 | 2253
Dow
nloa
ded
on 1
5 O
ctob
er 2
010
Publ
ishe
d on
10
Sept
embe
r 20
10 o
n ht
tp://
pubs
.rsc
.org
| do
i:10.
1039
/C0N
R00
281J
View Online
The extrapolation (Fig. 4b) of the straight line to a2 ¼ 0 gives
the value of the band-gap energy.
To further investigate absorption bands, the fluorescent
properties of the nanoparticles were measured using a steady-
state time-resolved spectrofluorometer at the wavelengths 260
and 360 nm for excitation scans and 350–600 nm for emission
scans (Fig. 5). We did not observe any prominent fluorescence
peaks for the as-prepared CoFe2O4–Cr2O3–SiO2 nanoparticles
Fig. 5 (a–b) Fluorescence emission spectra of CoFe2O4–Cr2O3–SiO2
particles excited at 260 and 360 nm; (c) emission spectra of quinine
sulphate in 0.1 mol L�1 H2SO4 solution and CoFe2O4–Cr2O3–SiO2
dispersion in water at 0.1 ABS excited at 370 nm; (d–e) Absorbance of the
nanocomposites in DMEM over a period of 24 h.
2254 | Nanoscale, 2010, 2, 2250–2256
(Fig. 5a). However, when the sample was annealed at 1000 �C,
a broad band at 460 nm appeared in the fluorescence spectrum,
(Fig. 5b). This was attributed to lattice defects, such as interval
atoms, displacement atoms and line defects resulting from grain
boundary diffusion between CoFe2O4 and Cr2O3. The presence
of defects in the nanocomposite is also supported by the
HRTEM images of the sample (Fig. 2c). Such lattice defects are
responsible for the luminescent properties of the nano-
composite.43
The fluorescent efficiency of the nanocomposite was measured
using quinine sulphate (FR ¼ 0.55)44 in 0.1 mol L�1 H2SO4
solution as a standard using the relationship:45
F ¼ FR
�IntARn2
IntRAn2R
�(3)
Where F is the quantum yield, Int is the area under the
emission peak (on a wavelength scale), A is absorbance at the
excitation wavelength of 370 nm, and n is the refractive index of
the sample (we have taken the value of nR ¼ 1.338,45 n ¼1.34639.46 FR ¼ 0.5547). The subscript R denotes the respective
values of the reference substance.
The fluorescence spectrum of the solutions were recorded in
a 20 mm fluorescence cuvette of constant slit width. In order to
minimize reabsorption effects, absorbances at 0.1 above the
excitation wavelength (at 370 nm) were used.48 The quantum-
yield of the FMNP sample was found to be 0.0354 (Fig. 5c),
which is appreciably good for bio-imaging.
The stability of the CoFe2O4–Cr2O3–SiO2 suspension was
inferred from optical absorbance measurements taken at
different intervals of time as studied by Gonz�alez-Caballero
et al.49 The optical absorbance was studied at 360 nm as a func-
tion of time. We scanned the entire range of wavelengths from
310 nm to 450 nm for different intervals of time. All suspensions
contained 0.1 g L�1 of CoFe2O4–Cr2O3–SiO2 particles in
a mixture of DMEM, Sodium bicarbonate and water. Fig. 5(d–e)
displayed the scanning spectra taken at 3 hour intervals up to 24
hours. From the spectra it was evident that there was no signif-
icant change in absorbance with time which revealed the stability
of the suspension of the ferrite particles. However, the overall
trend of A to decrease with time (DA ¼ 0.04), due to magnetic
interactions between the as-synthesized particles, demonstrates
their stability.
Fluorescence imaging experiments
The combination of nanoscale dimensions, ferromagnetic prop-
erties and fluorescence for these bifunctional nanoparticles has
prompted their use in medical imaging. Optical fluorescent
techniques have high spatial resolution in cellular imaging and
molecular event quantification. To demonstrate the utility of the
fluorescent nanocomposite, we sought to apply it to cellular
imaging. We have carried out our preliminary investigation using
human cervical cancer cells (HeLa) with a mean cell diameter of
14.6 � 0.8 mm as the model cell system and incorporated the
MFNP in the cell.
The as-synthesized SiO2-conjugated CoFe2O4–Cr2O3 nano-
particles were incubated with the HeLa cells, allowing an interac-
tion on the cell surface resulting in the nanoparticles attached to the
outer cell-membrane. The nanoparticles exhibited a surprisingly
This journal is ª The Royal Society of Chemistry 2010
Fig. 6 (a–c) TEM images of cultured HeLa cells; (d) SAED pattern
taken of the internal compartment of the cells; (e–f) pattern and fluo-
rescence image of cultured HeLa cells.
Table 2 Cell viability test for FMNPs
Entry Acontrol Atreated Cell viability Average
1 0.868 0.745 85.83 —2 0.855 0.755 88.30 —3 0.862 0.750 87.01 87.044 0.861 0.756 87.80 —5 0.865 0.746 86.24 —
Dow
nloa
ded
on 1
5 O
ctob
er 2
010
Publ
ishe
d on
10
Sept
embe
r 20
10 o
n ht
tp://
pubs
.rsc
.org
| do
i:10.
1039
/C0N
R00
281J
View Online
high level of cell internalization. While viewing the nanoparticle-
labeled cells using TEM, we were able to follow the nanoparticles
as they transported through the cell membrane (Fig. 6c) and into
internalized compartments (Fig. 6a–b) confirmed by the SAED
pattern (Fig 6d) taken of the cell compartments. The cellular
uptake of the nanoparticles was further confirmed by the inter-
cellular green fluorescence observed by morphology studies of the
HeLa cells under fluorescence microscopy using a confocal laser
scanning microscope (Fig 6e). We observed the morphological
changes in the HeLa cells after treatment with the nanoparticles by
fluorescence microscopic observation. The cells that were treated
with the FMNPs did not show any cell shrinkage or rounded
morphology. We observed a flattened morphology (Fig. 6e) of the
cells, which shows the non-toxicity of the nanoparticles.50
Cell viability experiments
To evaluate the biocompatibility of FMNPs as bio-imaging
probes, we investigated the cytotoxicity of FMNPs using a stan-
dard MTT assay.51 The cells (5 � 104 cells in 100 mL medium
well�1) were plated in 0.07% DMSO media as a control in 96-well
plates and were incubated for 24 h. After 24 h of growth, the
medium was exchanged for the medium that contained the
This journal is ª The Royal Society of Chemistry 2010
nanoparticles. The nanoparticle stock solution (150 mg mL�1)
was prepared in water. From the stock solution, aliquots of
nanoparticles were rapidly added to the culture medium. At the
end of the treatments, each well was treated with MTT (10 mL),
and after incubation for two hours, the absorption at 570 nm was
read with a microplate reader. The cell viability was calculated
using the following equation.
Cell viability ð%Þ ¼�
Atreated
Acontrol
�� 100 (1)
Where Atreated and Acontrol are the absorbance of the treated and
untreated cells, respectively. The cell viability date for concen-
trations of 150 mg mL�1 of the nanoparticles for different sets of
experiments are described in Table 2.
The FMNPs exhibited low toxicity (cell viability ¼ 87%)
towards HeLa cells even at a high concentration of 150 mg mL�1.
Conclusions
In conclusion, a combined sonochemical and co-precipitaion
method has been developed for the synthesis of core–shell
CoFe2O4–Cr2O3–SiO2 magnetic nanocomposites. The as-
prepared CoFe2O4–Cr2O3–SiO2 nanocomposites exhibit photo-
luminescence properties without the addition of any external
fluorescent marker. The fluorescent magnetic nanoparticles had
a typical diameter of 30 � 5 nm and a saturation magnetization
of 5.1 emu g�1 at room temperature. The fluorescent nano-
composites were further utilized for staining the cultured HeLa
cells for fluorescence imaging detection.
Acknowledgements
Financial support from DST (India) for the TEM facility at CIF,
IIT Guwahati (Grant No. SR/S5/NM-01/2005) and a Ramanna
Fellowship to P. Phukan (Grant No. SR/S1/RFPC-07/2006) is
gratefully acknowledged. The authors would also like to
acknowledge the support from IIT Guwahati for the vibrating
sample magnetometer, SEM and XRD facility. We thank
reviewers for their valuable suggestions.
References
1 Y. Kitamoto, S. Kantake, S. Shirashaki, F. Abe and M. Naoe,J. Appl. Phys., 1999, 85, 4708.
2 M. Pardavi-Horvath, H. Montiel, G. Alvarez, I. Betancourt,R. Zamorano and R. Valenzuela, J. Magn. Magn. Mater., 2000,171, 215.
3 M. Uhlen, Nature, 1989, 340, 733.4 D. G. Mitchell, J. Magn. Reson. Imaging, 1997, 7, 1.5 Y. Okuhata, Adv. Drug Delivery Rev., 1999, 37, 121.6 C. Bremer, V. Ntziachristos and R. Weissleder, Eur. Radiol., 2003, 13,
231.
Nanoscale, 2010, 2, 2250–2256 | 2255
Dow
nloa
ded
on 1
5 O
ctob
er 2
010
Publ
ishe
d on
10
Sept
embe
r 20
10 o
n ht
tp://
pubs
.rsc
.org
| do
i:10.
1039
/C0N
R00
281J
View Online
7 M. Doubrovin, I. Serganova, P. Mayer-Kuckuk, V. Ponomarev andR. G. Blasberg, Bioconjugate Chem., 2004, 15, 1376.
8 D. H. Han, H. L. Luo and Z. Yang, J. Magn. Magn. Mater., 1996,161, 376.
9 K. Giri, E. M. Kirkpatrick, P. Moongkhamklang, S. A. Majetich andV. G. Harris, Appl. Phys. Lett., 2002, 80, 2341.
10 H. R. Alexander Jr., T. S. Lawrence, S. A. Rosenberg, CancerPrinciples and Practice of Oncology, Williams, & Wilkins,Philadelphia, 2008.
11 M. A. G. Soler, T. F. O. Melo, S. W. da Silva, E. C. D. Lima,A. C. M. Pimenta, V. K. Garg, A. C. Oliviera and P. C. Morais,J. Magn. Magn. Mater., 2004, 272–276, 2357.
12 R. H. Misho and W. A. Murad, Thin Solid Films, 1989, 169, 235.13 Z. Pei and Y. Zhang, Mater. Lett., 2008, 62, 504.14 C. Tsang, IEEE Trans. Magn., 1989, MAG-25, 3672.15 R. D. Hempstead, S. Krongelb and D. A. Thompson, IEEE Trans.
Magn., 1978, 14, 521.16 S. Santra, P. Zhang, K. Wang, R. Tapec and W. Tan, Anal. Chem.,
2001, 73, 4988–4993.17 M. Bruchez Jr., M. Moronne, P. Gin, S. Weiss and A. P. Alivisatos,
Science, 1998, 281, 2013–2016.18 F. Wang and X. Liu, Chem. Soc. Rev., 2009, 38, 976; D. K. Chatterjee,
A. J. Rufaihah and Y. Zhang, Biomaterials, 2008, 29, 937;S. A. Hilderbrand, F. Shao, C. Salthouse, U. Mahmood andR. Weissleder, Chem. Commun., 2009, 4188; S. Jiang, Y. Zhang,K. M. Lim, E. K. W. Sim and L. Ye, Nanotechnology, 2009, 20,155101; M. Wang, C.-C. Mi, W.-X. Wang, C.-H. Liu, Y.-F. Wu,Z.-R. Xu, C.-B. Mao and S.-K. Xu, ACS Nano, 2009, 3, 1580;T. Zako, H. Nagata, N. Terada, A. Utsumi, M. Sakono,M. Yohda, H. Ueda, K. Soga and M. Maeda, Biochem. Biophys.Res. Commun., 2009, 381, 54; F. Vetrone, R. Naccache, A. J. de laFuente, F. Sanz-Rodr�ıguez, A. Blazquez-Castro, E. M. Rodriguez,D. Jaque, J. G. Sol�e and J. A. Capobianco, Nanoscale, 2010, 2, 495.
19 R. Hergt, et al., J. Phys.: Condens. Matter, 2006, 18, S2919.20 N. J. Durr, T. Larson, D. K. Smith, B. A. Korgel, K. Sokolov and
A. Ben-Yakar, Nano Lett., 2007, 7, 941.21 X. Hong, J. Li, M. J. Wang, J. J. Xu, W. Guo, J. H. Li, Y. B. Bai and
T. J. Li, Chem. Mater., 2004, 16, 4022.22 C. Jovaleki�c, M. Zdujic, A. Radakovic and M. Mitric, Mater. Lett.,
1995, 24, 365.23 K. V. P. M. Shafi, Y. Koltypin, A. Gedanken, R. Prozorov, J. Balogh,
J. Lendvai and I. Felner, J. Phys. Chem. B, 1997, 101, 6409.24 H. Tamura and E. Matijevic, J. Colloid Interface Sci., 1982, 90, 100.25 N. Moumen and M. P. Pileni, Chem. Mater., 1996, 8, 1128.26 C. Xiangfeng, D. L. Jiang, Y. Guo and C. M. Zheng, Sens. Actuators,
B, 2006, 120, 177.
2256 | Nanoscale, 2010, 2, 2250–2256
27 T. Sugimoto, Y. Shimotsuma and H. Itoh, Powder Technol., 1998, 85,96.
28 J. C. Hoh and I. I. Yaacob, J. Mater. Res., 2002, 17, 3105.29 E. Manova, B. Kunev, D. Paneva, I. Mitov, L. Petrov, C. Estournes,
C. D’Orl�eans, J.-H. Rehspringer and M. Kurmoo, Chem. Mater.,2004, 16, 5689.
30 T. Meron, Y. Rosenberg, Y. Lareah and G. Markovich, J. Magn.Magn. Mater., 2005, 292, 11.
31 E. Tirosh, G. Shemer and G. Markovich, Chem. Mater., 2006, 18,465.
32 T. Hyeon, Y. Chung, J. Park, S. S. Lee, Y.-W. Kim and B. H. Park,J. Phys. Chem. B, 2002, 106, 6831.
33 J. P. Zimmer, S. W. Kim, S. Ohnishi, E. Tanaka, J. V. Frangioni andM. G. Bawendi, J. Am. Chem. Soc., 2006, 128, 2526.
34 M. Yu, J. Lin and J. Fang, Chem. Mater., 2005, 17, 1783.35 B. D. Cullity, Elements of X-ray diffraction, Addison-Wesley
Publishing Co. Inc., Reading, MA, 1978, 363.36 V. M. Limaye, S. B. Singh, S. K. Date, D. Kothari, V. R. Reddy,
A. Gupta, V. Sathe, R. J. Choudhury and S. K. Kulkarni, J. Phys.Chem. B, 2009, 113, 9070.
37 M. Oca~na, J. Eur. Ceram. Soc., 2001, 21, 931.38 F. Nakagomi, S. W. da Silva, V. K. Garg, A. C. Oliveira and
P. C. Morais, J. Appl. Phys., 2007, 101, 09M514.39 A. Jordan, R. Scholz, P. Wust, H. Fahling and R. Felix, J. Magn.
Magn. Mater., 1999, 201, 413.40 R. E. Rosensweig, J. Magn. Magn. Mater., 2002, 252, 370.41 V. L. Colvin, M. C. Schlamp and A. P. Alivisatos, Nature, 1994, 370,
354.42 J. H. Park, J. Y. Kim, B. D. Chin, Y. C. Kim and O. O. Park,
Nanotechnology, 2004, 15, 1217.43 G. Zhang, W. Xu, Z. Li, W. Hu and Y. Wang, J. Magn. Magn.
Mater., 2009, 321, 1424.44 D. F. Eaton, Pure Appl. Chem., 1988, 60, 1107.45 M. S. Attia, M. M. H. Khalil, A. A. Abdel-Shafi, G. M. Attia,
S. Failla, G. Consiglio, P. Finocchiaro and M. S. A. Abdel-Mottaleb, Int. J. Photoenergy, 2007, 12530.
46 M. Daimon and A. Masumura, Appl. Opt., 2007, 46, 3811.47 W. H. Melhuish, J. Phys. Chem., 1961, 65, 229.48 S. Dhami, A. J. de Mello, G. Rumbles, S. M. Bishop, D. Phillips and
A. Beeby, Photochem. Photobiol., 1995, 61, 341.49 J. de Vicente, A. V. Delgado, R. C. Plaza, J. D. G. Dur�an and
F. Gonz�alez-Caballero, Langmuir, 2000, 16, 7954.50 A. Sahu, N. Kasoju and U. Bora, Biomacromolecules, 2008, 9,
2905.51 J. Yang, E.-K. Lim, H. J. Lee, J. Park, S. C. Lee, K. Lee, H.-G. Yoon,
J.-S. Suh, Y.-M. Huh and S. Haam, Biomaterials, 2008, 29, 2548.
This journal is ª The Royal Society of Chemistry 2010