# Effect of Electron Beam Irradiation on Optical Properties of Manganese Tungstate Nanoparticles

Authors: K. P. Priyanka; N. Aloysius Sabu; Anu Tresa Sunny; P. A. Sheena; Thomas Varghese
Journal: Journal of Nanotechnology
 (2013)

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## Abstract

Manganese tungstate (MnWO4) nanoparticles were synthesized at room temperature by chemical precipitation method. The effect of high energy electron beam (EB) irradiation on the optical properties of MnWO4 nanoparticles was investigated. The absorption spectra, photoluminescence intensity, and Raman bands of the irradiated samples were modified, which has been attributed to defects and particle size variation. The present investigation found that the beam irradiation is a new and efficient method to enhance the optical absorption performance and photoactivity of MnWO4 nanoparticles.


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## Body

## 1. Introduction

Nanostructured tungstate materials have aroused much interest because of their luminescence behaviour, structural properties, and potential applications. MnWO4 has bulk electrical conductivity, relatively low melting point, novel magnetic property, and photocatalytic property [1, 2]. The optical and luminescence properties of MnWO4 have received great attention as they are widely used as scintillating detectors in high-energy particle physics, rare-event searches, and medical diagnosis [3]. The electrical conductivity of MnWO4 is also sensitive to changes in humidity, thereby making it useful as a humidity sensor with potential applications like meteorology, medicine, food production, agriculture, and industrial and domestic environment [4, 5]. There are a number of processes used to synthesize nanocrystalline MnWO4, such as microwave-assisted synthesis [1], surfactant-assisted complexation-precipitation method [2], melt solution process [6], solvothermal route [7], aqueous salt metathesis reaction [8], sol-gel technique [4, 9], ambient template synthesis [10], and solid state metathetic approach [11].In the present work, manganese tungstate nanoparticles are synthesized by careful control of the reaction kinetics of aqueous precipitation. As-prepared MnWO4 nanoparticles are characterized by X-ray diffraction [XRD], transmission electron microscopy [TEM], UV-Visible absorption spectroscopy, photoluminescence [PL] spectroscopy and Raman spectroscopy. In addition, the optical properties of the pure and EB irradiated samples of MnWO4 nanoparticles were evaluated in context of the band gap.


## 2. Experimental Details

Manganese chloride (MnCl2·4H2O) (99.8%, Sigma Aldrich) and sodium tungstate (Na2WO4·2H2O) (99.9%, Alfa Aesar) were used without further purification for the synthesis of MnWO4. Distilled water was used in all synthesis procedures.


### 2.1. Preparation of the Samples

The synthesis procedures for the preparation of MnWO4 nanoparticles used in this work has been described elsewhere [12]. Nanocrystalline manganese tungstate samples were prepared by reacting aqueous solutions of manganese chloride and sodium tungstate (0.1 M each) at room temperature, keeping the pH=7. The precipitate formed was centrifuged, filtered, washed with distilled water a number of times, and dried in an oven to get fine powders of manganese tungstate. The obtained powder samples were calcined for 3 hours in a furnace at 450°C in an aerobic atmosphere. The flow chart showing the scheme of preparation of nanocrystalline MnWO4 is shown in Figure 1.Figure 1
The scheme of preparation of MnWO4 nanoparticles by chemical precipitation method.The MnWO4 samples were taken in microtubes and exposed to EB irradiation at a distance of 30 cm from the beam exit port. The samples were irradiated at a dose rate of 5 kGy and 10 kGy with an electron beam of 8 MeV energy obtained from a variable energy Microtron at Mangalore University, India. S1 is pure sample of MnWO4; S2 and S3 are irradiated samples with dose rates of 5 kGy and 10 kGy, respectively. The samples made significant modifications on their physical properties due to beam irradiation.


### 2.2. Characterization

The structural characteristics of the pure and irradiated manganese tungstate nanoparticles were studied by X-ray powder diffraction using Bruker D8 Advance X-ray diffractometer (λ=1.5406 Å) with CuKα radiation in 2θ range from 20° to 70°. From the XRD analysis all the peaks of MnWO4 were well matched with the X-ray pattern of JCPDS Card no. 80-0135. These analyses were carried out for the identification of the crystal phase and the estimation of the average crystallite size. The latter value was estimated from the Debye-Scherrer equation [9]. The Debye-Scherrer equation is given by
(1)t=0.9λβcosθ,
where λ is the X-ray wavelength, β is the full width at half-maximum (FWHM) of the peak, and θ is the Bragg’s angle.Transmission electron microscopy is a unique tool to get a direct image of the nanoparticles, revealing the distribution in the nanocrystal and on its surface. High magnification imaging with lattice contrast allows the determination of individual crystal morphology. For TEM studies, the MnWO4 powder was dispersed in ethanol using an ultrasonic bath. A drop of the suspension was placed on a copper grid coated with carbon film. After drying, the copper grid containing the nanoparticles was placed on a holder for the imaging process. TEM photographs of the pure nanocrystalline MnWO4 powder samples were taken using a Tecnai 30 G2 Stwin (model), FEI make 300 KV High Resolution Transmission Electron Microscope (HRTEM).The absorption spectra of the pure and irradiated samples in the range of 200–800 nm were recorded using a double beam UV-Visible Spectrophotometer (UV 2600 model, Shimadzu). For measurement, the nanoparticles were pressed into a thick pellet and placed at the entrance port of the integrating sphere using a sample holder. Calibration of the absorbance scale was done using standard reference materials.Photoluminescence spectroscopy is an effective way to investigate the electronic structure and optical characteristics of nanomaterials. This analytical technique reveals information such as surface defects and oxygen vacancies as well as the separation and recombination of photo-induced charge carriers [13]. PL spectra of the pure and EB irradiated samples of MnWO4 were measured at room temperature by a Fluoromax3 Spectrophotometer.Raman spectroscopy is a powerful tool for the investigation of the structural properties of nanoparticles because the variations in Raman spectra with decreases in particle size can be easily detected. Raman spectra of the pure and irradiated samples of MnWO4 were obtained at room temperature using a Bruker FRA 106/S Raman spectrometer with excitation line of 785 nm.


## 2.1. Preparation of the Samples

The synthesis procedures for the preparation of MnWO4 nanoparticles used in this work has been described elsewhere [12]. Nanocrystalline manganese tungstate samples were prepared by reacting aqueous solutions of manganese chloride and sodium tungstate (0.1 M each) at room temperature, keeping the pH=7. The precipitate formed was centrifuged, filtered, washed with distilled water a number of times, and dried in an oven to get fine powders of manganese tungstate. The obtained powder samples were calcined for 3 hours in a furnace at 450°C in an aerobic atmosphere. The flow chart showing the scheme of preparation of nanocrystalline MnWO4 is shown in Figure 1.Figure 1
The scheme of preparation of MnWO4 nanoparticles by chemical precipitation method.The MnWO4 samples were taken in microtubes and exposed to EB irradiation at a distance of 30 cm from the beam exit port. The samples were irradiated at a dose rate of 5 kGy and 10 kGy with an electron beam of 8 MeV energy obtained from a variable energy Microtron at Mangalore University, India. S1 is pure sample of MnWO4; S2 and S3 are irradiated samples with dose rates of 5 kGy and 10 kGy, respectively. The samples made significant modifications on their physical properties due to beam irradiation.


## 2.2. Characterization

The structural characteristics of the pure and irradiated manganese tungstate nanoparticles were studied by X-ray powder diffraction using Bruker D8 Advance X-ray diffractometer (λ=1.5406 Å) with CuKα radiation in 2θ range from 20° to 70°. From the XRD analysis all the peaks of MnWO4 were well matched with the X-ray pattern of JCPDS Card no. 80-0135. These analyses were carried out for the identification of the crystal phase and the estimation of the average crystallite size. The latter value was estimated from the Debye-Scherrer equation [9]. The Debye-Scherrer equation is given by
(1)t=0.9λβcosθ,
where λ is the X-ray wavelength, β is the full width at half-maximum (FWHM) of the peak, and θ is the Bragg’s angle.Transmission electron microscopy is a unique tool to get a direct image of the nanoparticles, revealing the distribution in the nanocrystal and on its surface. High magnification imaging with lattice contrast allows the determination of individual crystal morphology. For TEM studies, the MnWO4 powder was dispersed in ethanol using an ultrasonic bath. A drop of the suspension was placed on a copper grid coated with carbon film. After drying, the copper grid containing the nanoparticles was placed on a holder for the imaging process. TEM photographs of the pure nanocrystalline MnWO4 powder samples were taken using a Tecnai 30 G2 Stwin (model), FEI make 300 KV High Resolution Transmission Electron Microscope (HRTEM).The absorption spectra of the pure and irradiated samples in the range of 200–800 nm were recorded using a double beam UV-Visible Spectrophotometer (UV 2600 model, Shimadzu). For measurement, the nanoparticles were pressed into a thick pellet and placed at the entrance port of the integrating sphere using a sample holder. Calibration of the absorbance scale was done using standard reference materials.Photoluminescence spectroscopy is an effective way to investigate the electronic structure and optical characteristics of nanomaterials. This analytical technique reveals information such as surface defects and oxygen vacancies as well as the separation and recombination of photo-induced charge carriers [13]. PL spectra of the pure and EB irradiated samples of MnWO4 were measured at room temperature by a Fluoromax3 Spectrophotometer.Raman spectroscopy is a powerful tool for the investigation of the structural properties of nanoparticles because the variations in Raman spectra with decreases in particle size can be easily detected. Raman spectra of the pure and irradiated samples of MnWO4 were obtained at room temperature using a Bruker FRA 106/S Raman spectrometer with excitation line of 785 nm.


## 3. Results and Discussion

Figure2 shows the powder X-ray diffraction patterns of pure and EB irradiated samples of MnWO4 nanoparticles. From XRD patterns, the average particle size of the as-prepared and irradiated samples has been estimated using Debye-Scherrer equation. Average crystallite sizes obtained for samples S1, S2, and S3 are 26 nm, 23.4 nm, and 24.5 nm, respectively. The average crystallite size of sample S2 was decreased from 26 nm to 23.4 nm due to EB irradiation (5 kGy). However, the size of sample S3 was decreased only up to 24.5 nm after a dose of 10 kGy irradiation. The principal “d” values taken from the JCPDS file no. 80-0135 for MnWO4 are in close agreement with the observed “d” values. The XRD results showed that crystallite size and percentage of crystallinity decreased after irradiation. It confirms amorphization of the sample due to irradiation which is responsible for the change in optical properties. The results show that average particle size decreases with the EB irradiation dose and suggest the possible control of the size and the density of the MnWO4 nanoparticles by EB irradiation.Figure 2
XRD spectra of MnWO4 samples.All XRD patterns of MnWO4 samples correspond to a wolframite-type monoclinic structure, which is in agreement with the respective Inorganic Crystal Structure Database (ICSD) no. 67907. Unit cell parameters were a=0.4787 nm, b=0.5809 nm, c=0.4999 nm, and β=91.19° for sample S1, a=0.4843 nm, b=0.5869 nm, c=0.5035 nm, and β=91.23° for sample S2, and a=0.4823 nm, b=0.5826 nm, c=0.5021 nm, and β=91.22° for sample S3. All samples showed lattice parameters slightly larger than the calculated and experimental values of the bulk samples reported in the literature [14, 15]. This deviation might occur due to small particle size of the samples [16].TEM was used to further examine the particle size, crystallinity, and morphology of MnWO4 samples. TEM bright field images of MnWO4 nanoparticles (calcined at 450°C) are shown in Figure 3. It can be noted from the TEM image (Figure 3) that the particles are agglomerated and exhibit bar-like shape. Selected area electron diffraction (SAED) is shown in the inset of Figure 3, which clearly indicates that the MnWO4 nanoparticles were highly crystalline in nature. As can be seen from the TEM image, the average particle size is about 26 nm, which is in agreement with the crystallite size obtained from XRD data.TEM images of MnWO4 nanoparticles calcined at 450°C.
(a)
(b)Figure4 shows the UV-Visible absorbance spectra of pure and irradiated samples of MnWO4 nanoparticles. From the results, it can be observed that the absorption peak of samples S2 and S3 shifts towards the shorter wave length region. This blue shift in the absorption peak is the first-hand signature of significant size reduction of the nanoparticles resulting from EB irradiation. The blue shift in the absorption peak of sample S3 is less as compared to sample S2. It indicates that the size and size distribution of the particle increase beyond a certain EB irradiation dose level.Figure 4
UV-Visible absorption spectra of MnWO4 samples.The optical band gap values obtained from the absorption graphs for samples S1, S2, and S3 were 2.43 eV, 2.58 eV, and 2.51 eV, respectively. It is seen that the band gap of MnWO4 nanoparticles shifted from 2.43 to 2.58 eV as particle size reduced from 26 to 23.4 nm and from 2.43 to 2.51 eV as size reduced from 26 to 24.5 nm. This increase in the band gap might occur due to surface band bending with size reduction of the nanoparticles resulting from EB irradiation [16]. An additional advantage of size reduction is that the large surface area to volume ratio makes possible timely utilization of photo-generated carriers in interfacial processes [17]. Moreover, beam irradiation appeared to improve the optical absorption performance of MnWO4 nanoparticles. In addition, both pure and irradiated samples are useful for photocatalytic activities because their band gap energy values are comparable to the energy of visible or UV light photons.Table1 compares present experimental band gap values of MnWO4 with experimental and calculated values reported in the literature [14, 18, 19]. The present experimental values are higher as compared to literature values, which can be attributed to the reduction in particle size of the samples.Table 1
Comparison of experimental band gap values of MnWO4 with literature values.
Eg (eV)
Eg (eV)
Eg (eV)
Present work
Experimental
Theoretical
2.43 (S1)
2.5 [18, 19]
1.83 [14]
2.58 (S2)
2.37 [14]
2.51 (S3)Photoluminescence studies provide information relating to different energy states available between valence band and conduction band responsible for radiative recombination. Luminescence spectrum of MnWO4 nanoparticles with 293 nm excitation is shown in Figure 5. The PL emission spectra of the nonirradiated sample show emission bands at 423, 447, 460, 485, and 529 nm. These emission bands are attributed to the transition from the 1A1 ground state to the high vibration level of 1T2 and from the low vibration level of 1T2 to the 1A1 ground state within the tetragonal WO42- groups [20, 21].Figure 5
Room temperature PL spectra of MnWO4 samples.The pure and irradiated samples of MnWO4 could exhibit obvious PL signal with similar curve shapes (Figure 5). The PL spectra of irradiated samples were shown to have larger intensities relative to nonirradiated sample, which was thought to arise from defects and particle size variation [22]. Intermediate energy levels are formed with favourable characteristics due to EB irradiation, which are necessary for recombination process (electron/hole), responsible for the improvement of the PL emission at room temperature. During the excitation process, medium range defects in the monoclinic lattice caused by distortion of octahedral [WO6] clusters are responsible for the PL emission. Initially, some electrons from lower intermediate energy levels (oxygen—2p levels) near the valence band absorb the photon energy (hν) at this wavelength (λ=293 nm) and these energetic electrons are promoted to higher intermediate energy levels (tungsten—5d levels) located near the conduction band [21]. The energies generating from the deexcitation process are converted to photons (hν1). Several photons originating from the participation of different energy states during the electronic transitions are responsible for the intense PL emission.There was a small blue shift for PL spectra of the EB irradiated samples S2 and S3 (Figure5). The blue shift of band gap with size reduction could be due to surface band bending with surface structural modifications [16]. It can also be seen that PL spectra of the irradiated samples S2 and S3 were broadened. This broadening of MnWO4 nanoparticles might originate from the surface band bending and lattice expansion with particle size reduction caused by the EB irradiation [16].It can be seen in Figure5 that the PL intensity increases initially up to 5 kGy dose and then falls off at higher doses of irradiation. The initial increase is attributed to the increase in the trap states that give raise to the luminescence. The increase in PL intensity for an irradiated sample is attributed to the recombination of self-trapped excitons, which is a combined effect of defect centers generated by oxygen vacancies, small particle size, and increased absorption over the UV and visible range [21, 22]. The increase in PL intensity is also an indication of higher photocatalytic activity.When the EB irradiation dose rate is increased above a certain dose level, the particles agglomerate, thereby reducing the number of fluorophores. This possibly leads to a reduction in the fluorescence intensity (sample S3, Figure5). Further increase in the irradiation dose appears to have less effect on the trap states but slowly changes the size of the particle, thereby causing a shift in the fluorescence edge to longer wavelength side.Raman spectra for MnWO4 nanoparticles of pure and irradiated samples are shown in Figure 6. All the eighteen Raman modes were observed in the range 50–1200 cm−1 at room temperature. The most intense band observed at 886 cm−1 originated from the symmetric stretching vibration of a short terminal W–O bond, while the asymmetric stretching vibration of a short terminal W–O bond appeared at 775 cm−1. Other bands are contributed by asymmetric stretching vibration modes of longer W–O bond, symmetric stretching vibrations of longer W–O bond, deformation vibration of short W–O bonds, vibration modes of Mn-O, and interchain deformation modes and lattice modes [16, 23, 24]. It can be observed that Raman peaks were slightly shifted for the irradiated samples S2 and S3, and the shift was found large for the sample S2.Figure 6
Raman spectra of MnWO4 samples.It can be seen in Figure6 that Raman peaks of samples S2 and S3 were extremely broadened. The vibration mode for sample S2 at 886 cm−1 broadened from 15.5 to 30.2 cm−1, while for the sample S3, the line width broadened from 15.5 to 23.49 cm−1. The broadened Raman bands could be due to the quantum confinement effect [18]. Besides the quantum confinement, lattice expansion may also contribute to the broadened Raman peaks. The increased lattice volume for MnWO4 nanocrystals at smaller particle sizes would give the enlarged average length of W–O bonds, which may decrease the force constant of the W–O bond [25, 26]. As a result, Raman peaks of MnWO4 nanoparticles became broadened as particle size reduced.Present experimental Raman modes of MnWO4 nanoparticles are presented in Table 2 along with previous experimental and calculated values [23, 27]. Present results are slightly higher than the reported values, and this variation could be caused by the nanoscale size of the samples.Table 2
Comparison of Raman modes of MnWO4 with the literature.
Mode
Present values
Literature values [23, 27]
Calculated values [23, 27]
S1
S2
S3
Bg
90
79
82
89
95
Ag
130
119
123
129
129
Bg
162
151
154
160
165
Bg
168
157
161
166
171
Bg
182
171
174
177
183
Ag
205
193
198
206
226
Bg
276
265
269
272
278
Ag
259
242
252
258
264
Bg
297
290
293
294
296
Ag
330
317
320
327
338
B
g
′
361
349
354
356
373
A
g
*
399
393
395
397
389
Bg
514
506
508
512
509
A
g
*
547
528
535
545
548
B
g
*
675
633
642
674
662
A
g
*
702
688
695
698
694
B
g
*
776
762
769
774
775
A
g
*
888
878
882
885
858The structural characterization and optical studies of MnWO4 nanoparticles confirm the size reduction and structural modifications caused by the EB irradiation, which in turn result in blue shift in the absorption and PL spectra, and enhanced and broadened PL as well as Raman spectra.


## 4. Conclusions

MnWO4 nanoparticles were synthesized by simple chemical precipitation method, and the effect of high energy EB irradiation on their optical properties was studied in order to improve the optical absorption performance and photoactivity. The EB irradiation may have resulted in size reduction, which in turn caused an increase of the optical band gap as well as photoluminescence intensity and broadening of Raman bands. Furthermore, the data obtained here would seem to show that the method of EB irradiation may be considered as efficient means to enhance the optical response and photoactivity of MnWO4 nanoparticles for varied applications.



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