1 Introduction

Transition metal ferrites of the type AB2O4 with spinel structure such as ZnFe2O4, NiFe2O4 and CoFe2O4 have attracted considerable attention due to their magnetic, magnetoresistive and magneto-optical applications [1, 2]. Among different types of ferrites, CoFe2O4 has a wide range of applications in ferrofluids, magnetic storage devices, drug delivery, and magnetic resonance imaging (MRI) [3, 4]. It was found that the properties of ferrites are strongly influenced by their composition and morphology, which are extremely sensitive to the synthesis approach. However, various chemical methods have been developed to prepare CoFe2O4 nanostructures including sol–gel [5], hydrothermal [6] and microemulsion [7]. On the other hand, nano-sized bcc-CoFe2 alloy [8], metal-oleate complexes [9] and organometallic compounds [10] have been used as precursors for the preparation of CoFe2O4 nanostructures.

One of the main problems in the synthesis of transition metal ferrites such as CoFe2O4 is the self-condensation of the two metal precursors to form segregated Fe–O–Fe and Co–O–Co regions. To overcome this problem, the use of a new strategy has been developed in this work. So a novel single-source precursor including Fe and Co metals was applied for this purpose. Although the use of different complexes has been used to fabricate nano-sized materials [1117], complex of ethylenediamine, oxalate, Co3+ and Fe3+ formulated as [Co(en)3][Fe(ox)3] was first synthesized, and then applied as precursor to fabricate CoFe2O4 nanoparticles. Soli-state thermal decomposition of [Co(en)3][Fe(ox)3] complex was carried out at different temperatures from 400 to 800 °C. The final products were analyzed by scanning electron microscopy (SEM), transmission electron microscopy (TEM), X-ray powder diffraction (XRD), energy dispersive spectrometry (EDS), diffuse reflectance spectroscopy (DRS) and vibrating sample magnetometer (VSM).

2 Experimental

2.1 Materials

All chemical reagents were used without further purification. CoCl2·6H2O (98 %, Merck), Fe(NO3)3·6H2O (99.99 %, Merck), ethylenediamine (NH2CH2CH2NH2, 99.5 %, Merck), K2C2O4.H2O (99.5 %, Merck) and H2O2 (30 %, Aldrich) were used for the preparation of complexes.

2.2 Synthesis of [Co(en)3][Fe(ox)3] complex

In a 250 mL beaker, 25 mmol of CoCl2·6H2O was first dissolved in 25 mL of distilled water, and then 100 mmol of ethylenediamine was dropwise added into the CoCl2·6H2O solution. After that, 20 mL of H2O2 was added into the solution under magnetic stirring to oxidize the Co2+ ions to Co3+ ions. The beaker was placed in an ice bath to induce [Co(en)3]Cl3·3H2O crystals. Afterward, the orange crystals obtained were filtered on Buchner funnel. To prepare K3[Fe(ox)3]·3H2O complex, in a 250 mL beaker, 10 mmol of Fe(NO3)3·6H2O was dissolved in 50 mL of distilled water, and then 30 mmol of K2C2O4·H2O dissolved in 50 mL of distilled water was dropwise added into the Fe(NO3)3·6H2O solution under magnetic stirring. After evaporating of the solvent for 2 days, green K3[Fe(ox)3]·3H2O crystals were filtered on Buchner funnel. In order to synthesize [Co(en)3][Fe(ox)3] precursor, 10 mmol of the as-synthesized [Co(en)3]Cl3·3H2O and 10 mmol of K3[Fe(ox)3]·3H2O were separately dissolved in 50 mL of distilled water, and finally the K3[Fe(ox)3]·3H2O solution was gradually added into the [Co(en)3]Cl3·3H2O solution under magnetic stirring for 30 min to form [Co(en)3][Fe(ox)3] complex. At last, a brown precipitate was collected by filtration, washed three times with distilled water, and dried at 50 °C for 5 h in vacuum.

2.3 Synthesis of CoFe2O4 nanoparticles

In a typical synthesis, 0.5 g of the as-prepared [Co(en)3][Fe(ox)3] complex was loaded into a platinum crucible, and then it was placed in an oven and heated at a rate of 5 °C/min in air. Thermal decomposition process was carried out at different temperatures from 400 to 800 °C to fabricate cobalt ferrite nanoparticles. The preparation conditions of cobalt ferrites were illustrated in Table 1.

Table 1 Preparation conditions of cobalt ferrites synthesized by thermal decomposition

2.4 Characterization

Fourier transform infrared (FT-IR) spectra were recorded on Magna-IR spectrometer 550 Nicolet on KBr pellets in the range of 400–4000 cm−1. XRD patterns were collected on a diffractometer of Philips Company with X’pertpro monochromatized Cu Kα radiation (λ = 1.54 Å). TEM and SEM images were obtained on a TEM JEM-2100 transmission electron microscope with an accelerating voltage of 100 kV and HITACHI S4160 scanning electron microscope, respectively. The magnetic properties of the samples were studied by a vibrating sample magnetometer (VSM, BHV-55, Riken, Japan). Optical properties of the products were studied on an Ava-Spec-tec 2048 with Diffuse Reflectance Accessory. EDS analysis was studied by XL30 Philips microscope. Optical properties of the products were studied on Ava-Spec-tec 2048 with DRS.

3 Results and discussion

To determine the formation of the complex used as precursor, FT-IR spectra of the [Co(en)3]Cl3·3H2O, K3[Fe(ox)3]·3H2O and [Co(en)3][Fe(ox)3] complexes were taken and seen in Fig. 1. In the FT-IR spectrum of the [Co(en)3]Cl3·3H2O complex, the adsorption peaks in the regions of 1700–1500, 1052, 950–850 and 600–500 cm−1 are attributed to the NH2 bending, C–N stretching, CH2 rocking and Co–N stretching vibrations, respectively [18]. In the FT-IR spectrum of the K3[Fe(ox)3]·3H2O complex, the adsorption peaks at 1683, 1391 and 600–400 cm−1 can be related to the C=O stretching, C–O stretching and Fe–O stretching vibrations, respectively [19]. In the FT-IR spectrum of the [Co(en)3][Fe(ox)3] complex used as precursor, the adsorption peaks centered at 3430, 1705, 1661, 1374 and 1243 cm−1 can be assigned to the O–H stretching, C=O stretching, NH2 bending, C–O stretching and C–N stretching vibrations, respectively [19, 20]. In addition, the peaks observed in the range of 600–400 cm−1 can be related to the Co–N and Fe–O stretching vibrations. These observations proved the formation of the [Co(en)3][Fe(ox)3] complex. In the IR spectrum of the [Co(en)3][Fe(ox)3] complex, the adsorption peak corresponding to the stretching vibration of nitrate ions at 1350 cm−1 is not observed, indicating purity of the as-synthesized complex. In Table 2, all of the characteristic IR absorption bands for the [Co(en)3][Fe(ox)3] complex were illustrated.

Fig. 1
figure 1

FT-IR spectra of the as-prepared complexes: (a) [Co(en)3]Cl3, (b) K3[Fe(ox)3] and (c) [Co(en)3][Fe(ox)3]

Table 2 IR adsorption peaks of the as-synthesized [Co(en)3][Fe(ox)3] complex [1820]

Typical SEM images of the cobalt ferrites synthesized at different temperatures are seen in Fig. 2. When the [Co(en)3][Fe(ox)3] complex was calcined at 400 and 500 °C, very fine and homogeneous nanoparticles were formed. Particle sizes of the products synthesized at 400 and 500 °C are between 10–12 and 15–20 nm, respectively. By increasing the temperature from 500 to 600 °C, cobalt ferrite microstructures composed of nanoparticles were obtained. As shown in Fig. 2, by further increasing the temperature form 600 to 800 °C, the agglomeration of the cobalt ferrite nanoparticles increased. By comparing the SEM images presented in Fig. 2, it can be observed that by increasing the calcination temperature, the particle sizes of the products increased.

Fig. 2
figure 2

SEM images of the products synthesized at different temperatures

Chemical composition and purity of cobalt ferrites were investigated by EDS. The EDS spectrum of the product synthesized at 700 °C is seen in Fig. 3. The EDS spectrum clearly shows the presence of Co, Fe and O elements in the product. In addition, the EDS results give a rough atomic ratio Co:Fe:O as nearly 1:2:4, confirming the purity of the product.

Fig. 3
figure 3

EDS spectrum of the product synthesized at 700 °C

To obtain further insight into the details of the products, TEM micrographs of the product synthesized at 700 °C were taken and shown in Fig. 4. In the TEM images, the presence of aggregation nanoparticles with particle sizes in the range of 16–20 nm is visible.

Fig. 4
figure 4

a, b TEM images with different resolution for the product synthesized at 700 °C

The crystalline structures of the ferrite materials were investigated by XRD. Figure 5a–c shows XRD patterns of the products synthesized at 400, 700 and 800 °C, respectively. All the broad diffraction peaks in Fig. 5a, b can be indexed to cubic phase CoFe2O4 with space group of Fd3m and cell constants of a = b = c = 8.3900 Å (JCPDS: 01-1121). In Fig. 5c, some reflections with very low intensity are due to the presence of Co3O4 in the product, which formed at higher temperature. Therefore, pure phase cobalt ferrite is formed by calcination of the precursor at 700 °C. The crystallite sizes of the products synthesized at 700 and 800 °C calculated by the Scherrer formula are 14 and 29 nm, respectively. According to the XRD results, it was found that the calcination of the precursor at higher temperature (T > 700 °C) led to the formation of cobalt oxide.

Fig. 5
figure 5

XRD patterns of the products synthesized at (a) 400, (b) 700 and (c) 800 °C

The magnetic properties of the products were studied by a VSM. Figure 6a, b show the 300 K hysteresis loops of the products synthesized at 700 and 800 °C, respectively. The ferromagnetic nature of the products is clear. The coercive field (Hc), saturation magnetization (Ms) and remanent magnetization (Mr) values in Fig. 6 are illustrated in Table 3. The increased H c and M r values of the product synthesized at 800 °C may be related to the increased particle sizes. Although bulk CoFe2O4 exhibits a superparamagnetic character [21], the obtained results showed that the CoFe2O4 micro/nanostructures synthesized at 700 and 800 °C are ferromagnetic materials.

Fig. 6
figure 6

Magnetization curves of the products synthesized at a 700 and b 800 °C

Table 3 The coercive field (Hc), saturation magnetization (Ms) and remanent magnetization (Mr) values of the products synthesized at 700 and 800 °C

Optical properties of the products were studied by DRS. According to Eq. (1), absorption coefficient (α) is related to the incident photon energy (hv).

$$ \upalpha\left( {{\text{h}}v} \right) = B\left( {{\text{h}}v - {\text{E}}_{\text{g}} } \right)^{\text{n}} $$
(1)

where B is a constant and n is an index indicating the type of the transition. It is known that the value of n for direct band gap semiconductor is 1/2, and for indirect band gap semiconductor is 2 [22]. From extrapolation (αhv)2 versus (hv), band gap of cobalt ferrite can be estimated at (αhv)2 = 0, as shown in Fig. 7. As shown in Fig. 7a, b, the band gap (Eg) values of the products synthesized at 400 and 700 °C are about 3.2 and 2.1 eV, respectively. By considering the band gap values, it was found that by decreasing the particle size of the products, the Eg value increased due to the quantum confinement effects [23, 24]. The band gap of the CoFe2O4 nanoparticles with particle sizes about 10–12 nm is 3.2 eV that showed about 1.25 eV blue shift in comparison to its bulk type (1.95 eV).

Fig. 7
figure 7

Plot of (αhv)2 versus (hv) for the products synthesized at a 400 and b 700 °C

The choice of synthetic method is a key factors for the preparation of CoFe2O4 nanostructures. In Table 4, some applied methods and different conditions used for the synthesis of CoFe2O4 nanostructures were compared. By comparing the reported methods with this method, it was found that present method is simple, fast, and carried out in mild conditions. Additionally, the particle size of the products was smaller than that of other methods reported in Table 4 because of the presence of ethylenediamine and oxalate ligands in the structure of the as-used complex.

Table 4 Different methods compared for the preparation of CoFe2O4 nanostructures

4 Conclusions

In this work, CoFe2O4 micro/nanoparticles have been synthesized via a simple solid-state thermal decomposition process. For the first time, a new single-source precursor based on the coordination compound was applied to fabricate cobalt ferrite materials. In this method, calcination process of the [Co(en)3][Fe(ox)3] complex was carried out at different temperatures in the range of 400–800 °C. Based on the SEM images, it was found that by increasing the calcination temperature, the particle sizes of the products increased. In addition, optical properties of the final products indicated that the band gap of CoFe2O4 micro/nanoparticles is in the range of 2.1–3.2 eV.