# Structure and Magnetic Properties ofY3−xErxFe5O12 (x=0.2,1.0, and 2.0) Thin Films Prepared by Sol-Gel Method

Authors: Ramadan Shaiboub; Noor Baa'yah Ibrahim; Mustaffa Abdullah; Ftema Abdulhade
Journal: Journal of Nanotechnology
 (2011)

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## Abstract

NanoparticlesY3−xErxFe5O12 (x=0.2, 1.0, and 2.0) thin films were prepared by sol-gel method and treated at 800, 900, and 1000∘C, respectively, for 2 h. The films have single phase garnet structure and the sizes of particles are in the range of 44 to 83 nm. The magnetic measurements show that the saturation magnetization decreased with increasing of Er concentration for all samples treated at different annealing temperatures. The saturation magnetization increased with the particle size due to the enhancement of the surface spin effect. The coercivity initially decreased for x=1.0 and then increased for x=2.0 with increasing annealing temperature.


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## Body

## 1. Introduction

The rare-earth iron garnets (RIGs) have the general unit formula as R3Fe5O12, where R is either a trivalent rare- earth ion or yttrium. The garnets have eight formula units in a cubic unit cell. The cubic unit cells of RIGs have approximately the same lattice constant of the order of 12 Å´ [1], due to similar ionic radii of R3+ ions. Ionic distribution in garnet is represented as {R33+}[Fe23+](Fe33+)O12. The interaction between the Fe3+ ions in [a] and (d) sites is strongly antiferromagnetic due to a strong superexchange interaction. The magnetic moment of the rare-earth ions in the {c} sublattice couples antiparallel with the resultant moment of Fe3+ ions. YIG (Y3Fe5O12) is one of the common RIGs, which has attracted much attention in telecommunications and data storage industries due to their interesting magnetic and magneto-optic properties [2]. The resulting magnetic moment in YIG is due to the unequal distribution of Fe3+ ions in two different sublattices of [a] and (d). YIGs are also of scientific importance because of the wide variety of magnetic properties that can be obtained by substituting yttrium with a rare-earth (RE) metal [3–9]. Most of the previous studies have concentrated on the preparation of Bi- and Ce-doped YIG powders and films because of their high Faraday rotation coefficient [10–17]. Some studies have been carried out on Er-YIG powder nanoparticles [18–27].In this paper erbium is chosen because its ionic radius (1.03Å´) is slightly less than ionic radius of yttrium (1.04 Å´). Also, it has an extremely high verdet constant (~−11 × 10−2 min/Oe·cm) at (λ=600 nm) and large Bohr magneton (9.6 μB) [28]. This paper reports the influence of low and high concentration of Er3+ on the structure and magnetic properties of YIG thin films.


## 2. Experimental Method

The YIG precursor sol was prepared by a sol-gel method using reagent grade nitrates purchased from Aldrich, Milwaukee, Wis, USA. Yttrium nitrate hexahydrate (Y(NO3)3·6H2O, 99.95% purity), iron(III) nitrate nanohydrate (Fe(NO3)3·9H2O, 98% purity), and Erbium nitrate pentahydrate (Er(NO3)3·5H2O) were used as the raw materials. 2-methoxyethanol and acetic acid were used as solvents. Fe(NO3)3·9H2O and Y(NO3)3·6H2O were dissolved in the 2-methoxythanol and refluxed at 80°C for 3 hours. The Er(NO3)3·5H2O dissolved in acetic acid was added gradually into the Fe-Y solution. Then the refluxing process was continued for 3 hours. The pH value was adjusted in the range of 2-3. After cooling down to room temperature, the solution was stirred for 3 days. The gel was transformed into film on a quartz substrate using the spin coating technique. The rate of the spinning process was 3500 rpm, and it was done for 30 seconds. After the spinning process, the film was dried at room temperature. Then the heat treatment was carried out: initial heating at 350°C for 15 min to burn off the organic materials followed by heating at 800°C, 900°C, and 1000°C for 2 hours to crystallise the films.The characterizations were carried out using an X-ray diffractometer (Philips model Pw 3020 MRD x’pert pro) with a CuKα radiation (λ=1.54056 Å) to identify the phases and field emission scanning electron microscopic (FE-SEM model Zeiss Supra 55 vp) to determine the particle size and films thicknesses. The magnetic properties of the films were measured at room temperature using a vibrating sample magnetometer (VSM, LakeShore Cryotronics and 7400 Series).


## 3. Results and Discussion

### 3.1. Structural Properties

Figure1 shows the spectra for all samples. The XRD patterns reveal a single phase garnet structure and the crystallization had completely occurred at 800°C due to the good homogeneity of the gel prepared at pH = 2-3. This temperature is lower than that reported by Xu et al. [29]. However, increasing the temperature up to 1000°C does not give great influence to the sample crystallization. This is proved by the intensities ratio calculation shown in Table 1.Table 1
The average intensity ratios calculations forY3-xErxFe5O12 films.
x=0.2Temp. (°C)I
*Io1Io2Io3Io4Io1/I
*Io2/I
*Io3/I
*Io4/I
*(Io/I*) average80013566157094985210.450.520.370.380.4390014646137115015850.420.490.340.400.41100010474885584064230.470.530.390.400.45x=1.0Temp. (°C)I
*Io1Io2Io3Io4Io1/I
*Io2/I
*Io3/I
*Io4/I
*(Io/I*) average80010824785163973870.440.480.370.360.4190012365175704404560.420.460.360.370.40100013135486405155840.420.490.390.440.54x=2.0Temp. (°C)I
*Io1Io2Io3Io4Io1/I
*Io2/I
*Io3/I
*Io4/I
*(Io/I*) average80015796377425505200.400.470.350.330.3990011784865894414220.410.500.370.360.41100019667438046336020.380.410.320.310.36I*: highest intensity; Io1, Io2, Io3, and Io4: other peak intensities.XRD patterns ofY3-xErxFe5O12 films heated from 800 to 1000°C (a) x=0.2, (b) x=1.0, and (c) x=2.0.
(a)(b)(c)The average crystallite size was calculated according to the Scherrer’s formula(1)D=kλβcos⁡θ,
where D is the mean crystallite size, k (0.89) is the Scherrer constant, λ is X-ray wavelength (0.154252 nm), and β is the relative value of the full width at half maximum (FWHM) of the diffraction peak (420).The crystallite size for samples with the samex but treated at different temperature increased with increasing annealing temperature (Figure 2). It is observed that the films crystallites sizes are about the same at the same annealing temperatures as shown in Figure 3. The result is probably due to the similar ionic radii of Er3+ (1.03 Å´) and Y3+ (1.04 Å´) ions.Figure 2
Particle size dependence on the heating treatment forY3-xErxFe5O12 films.Figure 3
Particle size as a function of the Er concentration forY3-xErxFe5O12 films treated at different temperatures.


### 3.2. Magnetization

#### 3.2.1. In-Plane Saturation Magnetization (Ms) versus Particle Size (D)

Figure4 shows the variation in Ms with the average particle size for all samples. The results show that the Ms decreases with decreasing particle size for samples with the same x. A similar reduction in the magnetization was also reported for small particles of iron [30], α-Fe2O3 [31], BaFe12O9 [32], and MnFe2O4 [33]. This reduction can be related to the higher surface-to-volume ratio in the smaller particles, which results in the existence of nonmagnetic surface layer. Therefore, the Ms of the particles decreased as the particle sizes is reduced.Figure 4
Saturation magnetization with the average particle size for all films treated at different temperatures.


#### 3.2.2. Saturation Magnetization (Ms) versus Er Concentration (x)

The tetrahedral and octahedral cavities in YIG are occupied by Fe3+ ions and dodecahedral cavities are occupied by Y3+ ions. In this experiment, we substituted some Er3+ ions for Y3+ ions, so the ionic distribution can be written as {Y3-x3+Erx3+}[Fe23+](Fe33+)O122-, where, {}=c sub lattice, [  ] = a sub-lattice, and ( ) = d sub-lattice. Er3+ ion is magnetic (magnetic moment 9.6 μB) and Y3+ ion is nonmagnetic (magnetic moment 0 μB), so there are three magnetic sub-lattices: one (c) forms by the Er3+ ions occupying the dodecahedral sites, another [a] forms by Fe3+ ions occupying the octahedral sites, and the third (d) forms by the Fe3+ ions occupying the tetrahedral sites. The two iron sub-lattices are coupled antiferromagnetically by the superexchange interaction via the intervening O2− ions. The {c} sub-lattice is coupled antiferromagnetically with the tetrahedral sub-lattice. At room temperature, the three sub-lattice moments align along the [1 1 1] direction [34]. The net magnetic moment is M=Mc-|Md-Ma|.The variation of Ms with thex is shown in Figure 5. At different temperatures, Ms decreased with increasing x, which could be related to the fact that the magnetic moment of Er3+ ions aligns opposite to the effective moments formed by Fe3+ ions. With decreasing annealing temperatures the coercivity is initially decreased for x=1.0 and then increases for x=2.0 as shown in Figure 6.Figure 5
Saturation magnetization with Er concentration for all films treated at different temperatures.Figure 6
Coercivity with Er concentration for all films treated at different temperatures.


## 3.1. Structural Properties

Figure1 shows the spectra for all samples. The XRD patterns reveal a single phase garnet structure and the crystallization had completely occurred at 800°C due to the good homogeneity of the gel prepared at pH = 2-3. This temperature is lower than that reported by Xu et al. [29]. However, increasing the temperature up to 1000°C does not give great influence to the sample crystallization. This is proved by the intensities ratio calculation shown in Table 1.Table 1
The average intensity ratios calculations forY3-xErxFe5O12 films.
x=0.2Temp. (°C)I
*Io1Io2Io3Io4Io1/I
*Io2/I
*Io3/I
*Io4/I
*(Io/I*) average80013566157094985210.450.520.370.380.4390014646137115015850.420.490.340.400.41100010474885584064230.470.530.390.400.45x=1.0Temp. (°C)I
*Io1Io2Io3Io4Io1/I
*Io2/I
*Io3/I
*Io4/I
*(Io/I*) average80010824785163973870.440.480.370.360.4190012365175704404560.420.460.360.370.40100013135486405155840.420.490.390.440.54x=2.0Temp. (°C)I
*Io1Io2Io3Io4Io1/I
*Io2/I
*Io3/I
*Io4/I
*(Io/I*) average80015796377425505200.400.470.350.330.3990011784865894414220.410.500.370.360.41100019667438046336020.380.410.320.310.36I*: highest intensity; Io1, Io2, Io3, and Io4: other peak intensities.XRD patterns ofY3-xErxFe5O12 films heated from 800 to 1000°C (a) x=0.2, (b) x=1.0, and (c) x=2.0.
(a)(b)(c)The average crystallite size was calculated according to the Scherrer’s formula(1)D=kλβcos⁡θ,
where D is the mean crystallite size, k (0.89) is the Scherrer constant, λ is X-ray wavelength (0.154252 nm), and β is the relative value of the full width at half maximum (FWHM) of the diffraction peak (420).The crystallite size for samples with the samex but treated at different temperature increased with increasing annealing temperature (Figure 2). It is observed that the films crystallites sizes are about the same at the same annealing temperatures as shown in Figure 3. The result is probably due to the similar ionic radii of Er3+ (1.03 Å´) and Y3+ (1.04 Å´) ions.Figure 2
Particle size dependence on the heating treatment forY3-xErxFe5O12 films.Figure 3
Particle size as a function of the Er concentration forY3-xErxFe5O12 films treated at different temperatures.


## 3.2. Magnetization

### 3.2.1. In-Plane Saturation Magnetization (Ms) versus Particle Size (D)

Figure4 shows the variation in Ms with the average particle size for all samples. The results show that the Ms decreases with decreasing particle size for samples with the same x. A similar reduction in the magnetization was also reported for small particles of iron [30], α-Fe2O3 [31], BaFe12O9 [32], and MnFe2O4 [33]. This reduction can be related to the higher surface-to-volume ratio in the smaller particles, which results in the existence of nonmagnetic surface layer. Therefore, the Ms of the particles decreased as the particle sizes is reduced.Figure 4
Saturation magnetization with the average particle size for all films treated at different temperatures.


### 3.2.2. Saturation Magnetization (Ms) versus Er Concentration (x)

The tetrahedral and octahedral cavities in YIG are occupied by Fe3+ ions and dodecahedral cavities are occupied by Y3+ ions. In this experiment, we substituted some Er3+ ions for Y3+ ions, so the ionic distribution can be written as {Y3-x3+Erx3+}[Fe23+](Fe33+)O122-, where, {}=c sub lattice, [  ] = a sub-lattice, and ( ) = d sub-lattice. Er3+ ion is magnetic (magnetic moment 9.6 μB) and Y3+ ion is nonmagnetic (magnetic moment 0 μB), so there are three magnetic sub-lattices: one (c) forms by the Er3+ ions occupying the dodecahedral sites, another [a] forms by Fe3+ ions occupying the octahedral sites, and the third (d) forms by the Fe3+ ions occupying the tetrahedral sites. The two iron sub-lattices are coupled antiferromagnetically by the superexchange interaction via the intervening O2− ions. The {c} sub-lattice is coupled antiferromagnetically with the tetrahedral sub-lattice. At room temperature, the three sub-lattice moments align along the [1 1 1] direction [34]. The net magnetic moment is M=Mc-|Md-Ma|.The variation of Ms with thex is shown in Figure 5. At different temperatures, Ms decreased with increasing x, which could be related to the fact that the magnetic moment of Er3+ ions aligns opposite to the effective moments formed by Fe3+ ions. With decreasing annealing temperatures the coercivity is initially decreased for x=1.0 and then increases for x=2.0 as shown in Figure 6.Figure 5
Saturation magnetization with Er concentration for all films treated at different temperatures.Figure 6
Coercivity with Er concentration for all films treated at different temperatures.


## 3.2.1. In-Plane Saturation Magnetization (Ms) versus Particle Size (D)

Figure4 shows the variation in Ms with the average particle size for all samples. The results show that the Ms decreases with decreasing particle size for samples with the same x. A similar reduction in the magnetization was also reported for small particles of iron [30], α-Fe2O3 [31], BaFe12O9 [32], and MnFe2O4 [33]. This reduction can be related to the higher surface-to-volume ratio in the smaller particles, which results in the existence of nonmagnetic surface layer. Therefore, the Ms of the particles decreased as the particle sizes is reduced.Figure 4
Saturation magnetization with the average particle size for all films treated at different temperatures.


## 3.2.2. Saturation Magnetization (Ms) versus Er Concentration (x)

The tetrahedral and octahedral cavities in YIG are occupied by Fe3+ ions and dodecahedral cavities are occupied by Y3+ ions. In this experiment, we substituted some Er3+ ions for Y3+ ions, so the ionic distribution can be written as {Y3-x3+Erx3+}[Fe23+](Fe33+)O122-, where, {}=c sub lattice, [  ] = a sub-lattice, and ( ) = d sub-lattice. Er3+ ion is magnetic (magnetic moment 9.6 μB) and Y3+ ion is nonmagnetic (magnetic moment 0 μB), so there are three magnetic sub-lattices: one (c) forms by the Er3+ ions occupying the dodecahedral sites, another [a] forms by Fe3+ ions occupying the octahedral sites, and the third (d) forms by the Fe3+ ions occupying the tetrahedral sites. The two iron sub-lattices are coupled antiferromagnetically by the superexchange interaction via the intervening O2− ions. The {c} sub-lattice is coupled antiferromagnetically with the tetrahedral sub-lattice. At room temperature, the three sub-lattice moments align along the [1 1 1] direction [34]. The net magnetic moment is M=Mc-|Md-Ma|.The variation of Ms with thex is shown in Figure 5. At different temperatures, Ms decreased with increasing x, which could be related to the fact that the magnetic moment of Er3+ ions aligns opposite to the effective moments formed by Fe3+ ions. With decreasing annealing temperatures the coercivity is initially decreased for x=1.0 and then increases for x=2.0 as shown in Figure 6.Figure 5
Saturation magnetization with Er concentration for all films treated at different temperatures.Figure 6
Coercivity with Er concentration for all films treated at different temperatures.


## 4. Conclusion

The structure and magnetic properties ofY3-xErxFe5O12 films (x=0.2, 1.0 and 2.0) prepared by a sol-gel method have been reported. All the samples have only single phase garnet. The crystallization begins at 800°C, and as the heating temperature increases the obtained crystallite size is increased. At the same Er concentration, the saturation magnetization decreased as the particle size is reduced due to the influence of the magnetic domain structure and surface spin effect. The saturation magnetization decreased as the Er concentration is increased due to the opposite alignment between Er3+ ions and Fe3+ ions.



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*Source: 365378-2011-05-12.xml*