# Synthesis and Optical Characterization of  Mg1-xNixO Nanostructures

Authors: Nageswararao Budiredla; Ashok Kumar; Subhash Thota; Jitendra Kumar
Journal: ISRN Nanomaterials
 (2012)

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## Abstract

An attempt has been made here to synthesizeMg1-xNixO(0.01≤x≤0.10) nano-powders via sol-gel process. These powders are shown to possess an f.c.c. (NaCl-type) structure with a typical lattice parameter of 4.228(2) Å for “x”=0.01 when decomposition of dried oxalate gel product is carried out at 600°C for 2 h in air. Moreover, they exhibit  (i) clusters/agglomerates of nanosize particles and (ii) high BET specific surface area (123.0–135.5 m2/g). Also, the infrared absorption spectra reveal their strong affinity to water. The UV-Vis absorption peaks appearing at ~202 nm, 296 nm, and 379 nm are associated with oxygen defect centres and correspond to the electronic transitions (i) A11g→T11u (1s→2px, 2py, or 2pz), (ii) A11g→E1 (1s→2px, or 2py) and (iii) A11g→A11g (1s→2pz), respectively. The incorporation of Ni2+ ions causes some modifications in the energy levels and the optical  absorbance characteristics. The suppression of a strong broad emission peak at 440 nm and improvement of a weak band at ~400 nm in the photoluminescence (PL) spectrum arise due to decrease in population density of F22+  centres (or F+ dimmers) and emergence of additional F+centres, respectively with increase in nickel content.


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## Body

## 1. Introduction

Magnesium oxide (MgO) exhibits an f.c.c. (NaCl-type) crystal structure, high thermal stability, predominantly ionic nature, and insulating behaviour [1]. MgO has been extensively used in catalysis, toxic waste remediation, antibacterial materials, refractories, paints, and superconductors due to its unique optical, electronic, magnetic, thermal, mechanical, and chemical properties [2–8]. Recently, it has found promising application in plasma display panels [9]. Of particular interest is MgO nanopowder because of inherent size effects, for example, large surface area-to-volume ratio [10]. Various investigations have been undertaken earlier on its optical and electrical properties [2, 8, 11]. Surface anions with low coordination, considered to be chemically active sites, form excitons and give rise to specific optical transitions in the UV range [5, 8]. The processes usually used to synthesize MgO nanopowders include thermal evaporation, flame spray pyrolysis, laser vaporization, chemical gas phase deposition, combustion, aqueous wet chemical, vapor-phase transport, sol-gel, and hydrothermal reaction [5, 8, 12–15].The incorporation of another element into a parent phase (i.e., oxide matrix) leads to crystal defects (e.g., vacancies, interstitials, and antisites) which, in turn, can modify the useful characteristics [16, 17]. Recently, interest arose in transition metal and rare earth-doped oxides mainly due to their excellent luminescence efficiency and application in lasers, optical amplifiers, and plasma display panels [18–21]. In transition metal ions, the d–d absorptions are parity forbidden and therefore charge carriers get excited mainly from the host oxide. In such a situation, absorption can be improved by enhancing the energy transfer from host to doped transition metal ions and/or reducing the influence of defects. Also, the addition of coactive ions or charge compensators (e.g., silicon or nickel) sometime facilitates absorption process resulting in the enhancement of the luminescence intensity [20, 21]. Nickel is a well-known activator for many inorganic systems and produces white light by suitably adjusting the yellow and blue light emissions [20, 21].An attempt has been made here to study the effect of nickel doping on the crystal structure, morphology, particle size, optical absorption, and photoluminescence (PL) behaviour of MgO nanopowder with the objective of its possible application in optical devices. Sol-gel process has been chosen for synthesis because of its distinct advantage of being simple, cost effective,  low processing temperature, high purity, and chemical homogeneity [22, 23].


## 2. Experimental Details

For synthesis, magnesium nitrate hexahydrate [Mg(NO3)2·6H2O], nickel nitrate hexahydrate [Ni(NO3)2·6H2O], and oxalic acid [C2H2O4·2H2O] were used as precursors with ethanol as a solvent. First, 20 g of magnesium nitrate hexahydrate was added slowly to 200 mL of ethyl alcohol and stirred at 25°C until complete dissolution. Second, an appropriate amount of nickel nitrate hexahydrate was dissolved in 100 mL of ethyl alcohol similarly. Both these solutions were then mixed and oxalic acid solution (prepared in 200 mL of alcohol by taking metal to oxalate ion ratio as 1 : 1) added slowly with constant stirring to produce a thick white gel. The product was subsequently digested for 12 h, dried at 100°C for 24 h to yield presumably Ni-doped magnesium oxalate dihydrate which, in turn, was decomposed for 2 h each at 600, 800, and 1000°C to obtain Mg1-xNixO (0.01≤x≤0.10) powder. The flow chart of synthesis process is given in Scheme 1.Scheme 1
Flow chart of the synthesis process of  nickel doped magnesium oxide.To ascertain the condition of oxide formation, use was made of a thermogravimetry (TG) setup in the temperature range of 100–700°C. X-ray diffraction (XRD) patterns of various powder products were recorded with a diffractometer (Thermo Electron model ARL X’TRA) using the Cu Kα1 radiation (wavelength = 1.54062 Å) and used for identification of phase(s) and evaluation of the average grain size. The morphology was observed in a scanning electron microscope (FEI Model Quanta 200 HV SEM) using a secondary electron (SE) mode. For this, the powder was dispersed over a copper stub and coated with the gold film to avoid charging and improve the SE signal. Pore-size distribution and BET surface area data were deduced from nitrogen adsorption-desorption isotherms recorded with a gas adsorption analyzer (Micromeritics model ASPS-2400). Prior to the physisorption, the samples were heated at 120°C for 30 min in nitrogen atmosphere. A Fourier transform infrared (FTIR) spectrometer (BRUKER Vertex-70) was used for detection of hydroxyl (−OH) and other groups in oxalates and –OH– stretching mode in oxide samples. For optical absorption measurements, a double beam UV-VIS-NIR spectrophotometer (Varian Cary 5000) was employed in the wavelength range of 200–800 nm. Further, the photoluminescence (PL) spectra were obtained with a Spex Fluorolog II Spectrophotometer at the excitation wavelength of 350 nm.


## 3. Results and Discussion

### 3.1. Formation of Nickel Containing MgO

Thermogravimetric analysis (TGA) of the sol-gel product was undertaken to gather information about its thermal stability and the formation of nickel containing MgO powders. For this, weight of sol-gel product (initially, 0.384 g) has been monitored by raising its temperature at a rate of 4°C/min from 100 to 700°C in air. Figure1 shows the weight percentage (W%) and derivative (-dW%/dT) versus temperature plots of sample containing Ni/(Ni+Mg) atomic ratio of 0.01, dried at 100°C for 24 h. Accordingly, the first weight loss of ~22.5% occurs in the temperature range of 160–244°C with peak at 218°C. This weight loss can be attributed to removal of crystallizing water of presumably mixed oxalate (Mg, Ni) C2O4·2H2O, which is 24.4 wt% and follow the reaction
(1)(Mg,Ni)C2O4·2H2O→(Mg,Ni)C2O4+2H2O(↑).
In the second stage, the weight loss of 51.6 wt% observed in the temperature range of 440–520°C (peak at 497°C) matches reasonably well with the evolution of CO and CO2 (amounting to ~48.9%) from the anhydrous oxalate, (Mg, Ni) C2O4. The overall reaction can be written as
(2)(Mg,Ni)C2O4→440-520C°(Mg,Ni)O+CO(↑)+CO2(↑).
The slight discrepancy in weight loss can be understood if removal of water is partial in the first stage and the remaining amount gets evolved later in the temperature range of 440–520°C. No apparent weight change (i.e., loss or gain) occurs beyond 520°C. The final product reduced to about 26% of the initial weight. Accordingly, the decomposition temperature of 600°C or above can be chosen for the formation of a stable compound.Figure 1
Percentage weight (W%) versus temperature (T) and (-dW%/dT) versus T plots of dried sol-gel product containing [Ni/(Ni+Mg)] atomic ratio of 0.01.X-ray diffraction (XRD) patterns of the sol-gel products dried at 100°C for 24 h are shown in Figure2. Their analysis suggests the emergence of a phase similar to magnesium oxalate dihydrate [α-MgC2O4·2H2O] having monoclinic structure with lattice parameters a=12.68 Å, b=5.391 Å, c=9.977 Å, β=129.82, and Z=4 [JCPDS # 26-1223]. Further, there is no evidence to indicate the presence of nickel or nickel compound in the product. Figure 3 shows XRD patterns of Mg1-xNixO (x=0.01,0.05, and 0.10) powders obtained by decomposition of respective dried sol-gel oxalate for 2 h each at 600°C. These patterns are similar in nature and correspond to f.c.c. (NaCl-type) structure of MgO [JCPDS # 45-0946] with marginal variation in the lattice parameter, typical value being 4.228±0.002 Å for powder with nickel content (x) equal to 0.01. Moreover, the patterns contain no evidence of any secondary phase. The changes in the lattice parameters are marginal and are on expected line as Ni2+ ions occupy Mg2+ sites in MgO and both the ions have nearly the same size (ionic radii of Ni2+ and Mg2+ in octahedral configuration being 0.69 and 0.72 Å, resp.). The average grain size has been determined from the Scherrer formula, D=0.9λ/βcosθ (where λ is the wavelength of X-rays and β is the full width at half maximum of the diffraction peak at Bragg angle θ), with 200 peak and using silicon as standard to make correction for the instrumental broadening. The values obtained are in the range 11.4–12.6 nm for Mg1-xNixO (x=0.01,0.05, and 0.10).Figure 2
XRD patterns of the sol-gel products dried at 100°C for 24 h showing emergence of a monoclinic phase, similar toα-MgC2O4·2H2O, for [Ni/(Ni+Mg)] atomic ratio (a) 0.01, (b) 0.05, and (c) 0.10.Figure 3
XRD patterns ofMg1-xNixO nanopowders formed by decomposition of respective oxalates at 600°C for 2 h each for x equal to (a) 0.01, (b) 0.05, and (c) 0.10 indicating formation of f.c.c. (NaCl-type) phase similar to magnesium oxide.The XRD patterns (not shown here) ofMg1-xNixO (x=0.01) powder samples obtained by decomposition of sol-gel product in air for 2 h each at 600, 800, and 1000°C reveal slight decrease in the lattice parameter with increase of the decomposition temperature; values being 4.228, 4.223, and 4.212±0.002Å for 600, 800, and 1000°C, respectively. Clearly, the lattice parameter is approaching the bulk value of MgO and peaks become sharper and stronger with increase in decomposition temperature. This is consistent with previous studies on pure MgO nanopowders [5].The scanning electron micrographs in secondary electron (SE) mode of magnesium oxalate dihydrate containing different nickel content, that is, [Ni/(Ni+Mg)] atomic ratio (x) as 0.01, 0.05, and 0.10, obtained after drying/digesting the sol-gel product at 100°C for 24 h are shown in Figures 4(a), 4(b), and 4(c). These images reveal the emergence of nanorods/nanostrips with varied diameter/width and length in the range 76–120 nm and 312–436 nm, respectively. Also, a few spherical nanoparticles are visible at places independently or within rods. The decomposition of sol-gel products at 600°C for 2 h invariably yields spherical clusters/agglomerates of nanosize particles of nickel doped magnesium oxide (Figures 4(d), 4(e), and 4(f)). Thus, nickel doping in MgO causes little morphological changes in the nature of particles/clusters/agglomerates in comparison to other reports [24, 25].Scanning electron micrographs (a, b, and c) of sol-gel products presumably of oxalates after drying at 100°C for 24 h and (d, e, and f) of corresponding oxide powders, formed by decomposition at 600°C for 2 h each in air for Ni/(Ni+Mg) atomic ratio (x) equal to 0.01, 0.05, and 0.10, respectively.
(a)
(b)
(c)
(d)
(e)
(f)The values of BET surface area ofMg1-xNixO (0.01≤x≤0.10) powders formed by decomposition of respective oxalates at 600°C for 2 h in air as deduced from nitrogen adsorption isotherms are within 123.0–135.5 m2/g. The corresponding average particle diameter (d) has been determined from the formula d=6/(s·ρ), where s stands for BET specific area and ρ represents the material density (which varies with composition); the values of (d) lie in the range 12.0–12.7 nm. These results suggest that nickel doping up to ~10 at% has negligible/no effect on the average particle size. However, the values of (d) match reasonably well with the average crystallite size data obtained from XRD for Mg1-xNixO powders. The high BET surface area and small average particle size are expected to improve the characteristics of Mg1-xNixO powders appreciably to make them suitable for applications in plasma display panels [26, 27].


### 3.2. Optical Characteristics

#### 3.2.1. Infrared Absorption

The FTIR spectra of sol-gel-derived oxalate samples of Ni/(Ni+Mg) atomic ratios (x) 0.01, 0.05, and 0.10 are shown in Figure 5. The broad absorption band around 3408 cm−1 is in fact composed of several peaks in the wave number range of 3100–3700 cm−1. These correspond to the –OH group stretching vibrations and provide evidence for the presence of chemically bound water. The deformational mode of water usually seen around 1650 cm−1 is, however, masked by the doublet at 1667 cm−1. The other sharp absorption peaks at 1373 and 1325 cm−1 are assigned to νs (C–O) and δ  (OC=O) modes. While weak band at 696 cm−1 is attributed to bending mode of O=C=O and/or liberation of water, a peak at 501 cm−1 is assigned to ν (Mg–O) + ν (C–C) modes [5, 28, 29].Figure 5
Fourier transform infrared (FTIR) spectra of sol-gel products, each dried at 100°C for 24 h in air, with Ni/(Ni+Mg) atomic ratio equal to (a) 0.01, (b) 0.05, and (c) 0.10.Figure6 shows the FTIR transmittance spectra of Mg1-xNixO (x=0.01,0.05, and 0.10) produced by decomposition of Ni-doped α-MgC2O4·2H2O at 600°C for 2 h in air. These contain signatures of adsorption and chemisorption of water. The sharp peak centred around 3699 cm−1 indicates the presence of hydroxyl group at the low-coordination sites or defects [5, 28, 29]. The absorption band in the wave number range 3672–3000 cm−1 is quite broad and can be assigned to –OH-stretching mode of adsorbed H2O on the surface of oxide crystallites. The absorption band in the range of 1300–1750 cm−1 is related to hydroxyl groups of molecular water. Since the spectra were not recorded in situ, the products could reabsorb some water from the ambient.Figure 6
Fourier transform infrared (FTIR) spectra ofMg1-xNixO powders, obtained by decomposition of respective oxalates at 600°C for 2 h each in air for x equal to (a) 0.01, (b) 0.05, and (c) 0.10.


#### 3.2.2. UV-VIS Absorption

The optical absorption spectra ofMg1-xNixO (x=0.01,0.5,0.1) powders, obtained by decomposition of dried sol-gel product at 600°C for 2 h in air, in the wavelength range of 200–800 nm are shown in Figure 7. The optical absorption of pure MgO prepared similarly has already been presented elsewhere [5]. Table 1 summarises the optical data in terms of peak energy and absorbance. In pure MgO, a magnesium atom donates two electrons from its 3s2-orbitals to 2p-orbitals of oxygen. An energy band gap is thus created between the valence band (oxygen 2p) and conduction band (magnesium, 3s). The known value of energy band gap (Eg) of MgO is about 7.8 eV [5, 27]. A strong absorption band near 202 nm and two other peaks around 296 and 379 nm appear in pure MgO. The former corresponds to (A11g→T1u1) transition from 3P2 state of oxygen (O2−) to 1S0 state of magnesium (Mg2+). The other two peaks at 296 and 379 nm are assigned to A11g→E1 (1s→2px or 2py) and A11g→A11g (1s → 2pz) transitions of oxygen defect centres [5, 30]. With incorporation of Ni2+ ions in MgO, absorption peaks shift slightly, and correspond to improved absorbance  (Table 1, Figure 7). Since no additional band appears, Ni2+ ion is possibly substituting Mg2+ ion in MgO but somehow influencing the absorbance significantly.Table 1
Optical absorption peaks observed inMg1–xNixO nanopowders, prepared by decomposition of dried sol-gel-derived oxalate at 600°C for 2 h each in air for nickel content
(x) = 0, 0.01, 0.05, and 0.10.
No.
x
Peak 1
Peak 2
Peak 3
E (eV)
Abs.
E (eV)
Abs.
E (eV)
Abs.
1*
0
6.13+
0.97
4.20#
0.20
3.27†
0.24
2
0.01
6.13
0.98
4.27
0.27
3.35
0.30
3
0.05
6.20
1.15
4.33
0.36
3.22
0.33
4
0.10
6.10
1.09
4.26
0.45
3.09
0.37
*[5].
+ 1
A
1
g
→
1
T
1
u
(
1
s
→
2
p
x
,
2
p
y
,
or
2
p
z
).
# 1
A
1
g
→
1
E
(
1
s
→
2
p
x
or
2
p
y
).
† 1
A
1
g
→
1
A
1g
(
1
s
→
2
p
z
).Figure 7
Optical absorption spectra ofMg1-xNixO powders, obtained by decomposition of respective oxalates at 600°C for 2 h each in air for x equal to (a) 0.01, (b) 0.05, and (c) 0.10.


#### 3.2.3. Photoluminescence (PL) Behaviour

Photoluminescence (PL) spectra ofMg1-xNixO (x=0.01,0.05,0.10) powders, obtained by decomposition of respective oxalates at 1000°C for 2 h in air, with the excitation wavelength of 350 nm are shown in Figure 8. They exhibit a luminescence band centred at 440 nm which becomes broad and shifts slightly towards a higher wavelength (or lower energy) when Ni content (x) increases in MgO matrix. Further, a new emission peak begins to develop near 400 nm and its intensity increases progressively with nickel concentration. This observation suggests changes in the symmetry and vibrational modes around the luminescent centres with nickel doping. Since there is small difference and  ionic radius of Ni2+ (0.69 Å) being smaller than Mg2+ (0.72 Å), the former is possibly substituting the latter in MgO.Figure 8
Photoluminescence (PL) spectra of theMg1-xNixO powders for x equal to (a) 0.01, (b) 0.05, and (c) 0.10.Pure MgO sample prepared similarly exhibits two emission peaks (strong around 440 nm and weak at 395 nm) with the excitation wavelength of 350 nm and are assigned toB21u→A1g and T21u→A21g transitions, respectively [8]. Moreover, their origin lies with the existence of F22+ (or F+ dimers) and F+-colour centres, respectively, F+ being oxygen vacancy retaining one electron [8]. This fact in conjunction with the above results indicates that partial substitution of Mg2+ by Ni2+ ions causes decrease of F+ dimers with simultaneous increase of F+-defect centres in MgO. The process can occur in two ways, namely, F+ dimer either splits into two F+ centres or converts into one F+ centre with transfer of extra electron rendering Ni2+→Ni1+conversion. It may be mentioned that Ni2+ ion has an empty (eg) low-spin orbital.Photoluminescence studies of pure MgO nanocrystals with excitation wavelength of 273 nm have revealed a broad emission band centred around 350 nm arising due to oxygen vacancies [13, 30]. In Dy3+-doped MgO, emission peaks appear at 480 nm and 575 nm due to 4F9/2 − 6H15/2 and 4F9/2 − 6H13/2 transitions of dysprosium [18]. In fact, Dy3+-ions encounter difficulty in substitution because of their large size (ionic radii being 0.91 Å against 0.72 Å of Mg2) and therefore lie essentially on the surface or in the grain boundaries giving its own PL emission at 575 nm. On the other hand, Ni2+ ions can assume Mg2+ sites easily and influence the nature of emission. As a consequence, the peak at 440 nm diminishes and that near 400 nm rises due to decrease in F22+ centres (or dimers) and formation of additional F+ centres occurring in MgO.Upon substitution, Ni2+ ion occupies an octahedral void in MgO and so is coordinated with six oxygen ions. The energy level diagram of Ni2+ (3d8) ion suggests three major thermoradiative energy transitions, 1A1→1E (1117 nm, 1.110 eV), 3T2→3A2 (1256 nm, 0.987 eV), and 1T2→1E (1414 nm, 0.877 eV) at 1300–1400°C. Thus, Ni-doped MgO may also serve as a potential emitter for thermophotovoltaic (TPV) generators [20, 21]. Work is in progress in this direction.


## 3.1. Formation of Nickel Containing MgO

Thermogravimetric analysis (TGA) of the sol-gel product was undertaken to gather information about its thermal stability and the formation of nickel containing MgO powders. For this, weight of sol-gel product (initially, 0.384 g) has been monitored by raising its temperature at a rate of 4°C/min from 100 to 700°C in air. Figure1 shows the weight percentage (W%) and derivative (-dW%/dT) versus temperature plots of sample containing Ni/(Ni+Mg) atomic ratio of 0.01, dried at 100°C for 24 h. Accordingly, the first weight loss of ~22.5% occurs in the temperature range of 160–244°C with peak at 218°C. This weight loss can be attributed to removal of crystallizing water of presumably mixed oxalate (Mg, Ni) C2O4·2H2O, which is 24.4 wt% and follow the reaction
(1)(Mg,Ni)C2O4·2H2O→(Mg,Ni)C2O4+2H2O(↑).
In the second stage, the weight loss of 51.6 wt% observed in the temperature range of 440–520°C (peak at 497°C) matches reasonably well with the evolution of CO and CO2 (amounting to ~48.9%) from the anhydrous oxalate, (Mg, Ni) C2O4. The overall reaction can be written as
(2)(Mg,Ni)C2O4→440-520C°(Mg,Ni)O+CO(↑)+CO2(↑).
The slight discrepancy in weight loss can be understood if removal of water is partial in the first stage and the remaining amount gets evolved later in the temperature range of 440–520°C. No apparent weight change (i.e., loss or gain) occurs beyond 520°C. The final product reduced to about 26% of the initial weight. Accordingly, the decomposition temperature of 600°C or above can be chosen for the formation of a stable compound.Figure 1
Percentage weight (W%) versus temperature (T) and (-dW%/dT) versus T plots of dried sol-gel product containing [Ni/(Ni+Mg)] atomic ratio of 0.01.X-ray diffraction (XRD) patterns of the sol-gel products dried at 100°C for 24 h are shown in Figure2. Their analysis suggests the emergence of a phase similar to magnesium oxalate dihydrate [α-MgC2O4·2H2O] having monoclinic structure with lattice parameters a=12.68 Å, b=5.391 Å, c=9.977 Å, β=129.82, and Z=4 [JCPDS # 26-1223]. Further, there is no evidence to indicate the presence of nickel or nickel compound in the product. Figure 3 shows XRD patterns of Mg1-xNixO (x=0.01,0.05, and 0.10) powders obtained by decomposition of respective dried sol-gel oxalate for 2 h each at 600°C. These patterns are similar in nature and correspond to f.c.c. (NaCl-type) structure of MgO [JCPDS # 45-0946] with marginal variation in the lattice parameter, typical value being 4.228±0.002 Å for powder with nickel content (x) equal to 0.01. Moreover, the patterns contain no evidence of any secondary phase. The changes in the lattice parameters are marginal and are on expected line as Ni2+ ions occupy Mg2+ sites in MgO and both the ions have nearly the same size (ionic radii of Ni2+ and Mg2+ in octahedral configuration being 0.69 and 0.72 Å, resp.). The average grain size has been determined from the Scherrer formula, D=0.9λ/βcosθ (where λ is the wavelength of X-rays and β is the full width at half maximum of the diffraction peak at Bragg angle θ), with 200 peak and using silicon as standard to make correction for the instrumental broadening. The values obtained are in the range 11.4–12.6 nm for Mg1-xNixO (x=0.01,0.05, and 0.10).Figure 2
XRD patterns of the sol-gel products dried at 100°C for 24 h showing emergence of a monoclinic phase, similar toα-MgC2O4·2H2O, for [Ni/(Ni+Mg)] atomic ratio (a) 0.01, (b) 0.05, and (c) 0.10.Figure 3
XRD patterns ofMg1-xNixO nanopowders formed by decomposition of respective oxalates at 600°C for 2 h each for x equal to (a) 0.01, (b) 0.05, and (c) 0.10 indicating formation of f.c.c. (NaCl-type) phase similar to magnesium oxide.The XRD patterns (not shown here) ofMg1-xNixO (x=0.01) powder samples obtained by decomposition of sol-gel product in air for 2 h each at 600, 800, and 1000°C reveal slight decrease in the lattice parameter with increase of the decomposition temperature; values being 4.228, 4.223, and 4.212±0.002Å for 600, 800, and 1000°C, respectively. Clearly, the lattice parameter is approaching the bulk value of MgO and peaks become sharper and stronger with increase in decomposition temperature. This is consistent with previous studies on pure MgO nanopowders [5].The scanning electron micrographs in secondary electron (SE) mode of magnesium oxalate dihydrate containing different nickel content, that is, [Ni/(Ni+Mg)] atomic ratio (x) as 0.01, 0.05, and 0.10, obtained after drying/digesting the sol-gel product at 100°C for 24 h are shown in Figures 4(a), 4(b), and 4(c). These images reveal the emergence of nanorods/nanostrips with varied diameter/width and length in the range 76–120 nm and 312–436 nm, respectively. Also, a few spherical nanoparticles are visible at places independently or within rods. The decomposition of sol-gel products at 600°C for 2 h invariably yields spherical clusters/agglomerates of nanosize particles of nickel doped magnesium oxide (Figures 4(d), 4(e), and 4(f)). Thus, nickel doping in MgO causes little morphological changes in the nature of particles/clusters/agglomerates in comparison to other reports [24, 25].Scanning electron micrographs (a, b, and c) of sol-gel products presumably of oxalates after drying at 100°C for 24 h and (d, e, and f) of corresponding oxide powders, formed by decomposition at 600°C for 2 h each in air for Ni/(Ni+Mg) atomic ratio (x) equal to 0.01, 0.05, and 0.10, respectively.
(a)
(b)
(c)
(d)
(e)
(f)The values of BET surface area ofMg1-xNixO (0.01≤x≤0.10) powders formed by decomposition of respective oxalates at 600°C for 2 h in air as deduced from nitrogen adsorption isotherms are within 123.0–135.5 m2/g. The corresponding average particle diameter (d) has been determined from the formula d=6/(s·ρ), where s stands for BET specific area and ρ represents the material density (which varies with composition); the values of (d) lie in the range 12.0–12.7 nm. These results suggest that nickel doping up to ~10 at% has negligible/no effect on the average particle size. However, the values of (d) match reasonably well with the average crystallite size data obtained from XRD for Mg1-xNixO powders. The high BET surface area and small average particle size are expected to improve the characteristics of Mg1-xNixO powders appreciably to make them suitable for applications in plasma display panels [26, 27].


## 3.2. Optical Characteristics

### 3.2.1. Infrared Absorption

The FTIR spectra of sol-gel-derived oxalate samples of Ni/(Ni+Mg) atomic ratios (x) 0.01, 0.05, and 0.10 are shown in Figure 5. The broad absorption band around 3408 cm−1 is in fact composed of several peaks in the wave number range of 3100–3700 cm−1. These correspond to the –OH group stretching vibrations and provide evidence for the presence of chemically bound water. The deformational mode of water usually seen around 1650 cm−1 is, however, masked by the doublet at 1667 cm−1. The other sharp absorption peaks at 1373 and 1325 cm−1 are assigned to νs (C–O) and δ  (OC=O) modes. While weak band at 696 cm−1 is attributed to bending mode of O=C=O and/or liberation of water, a peak at 501 cm−1 is assigned to ν (Mg–O) + ν (C–C) modes [5, 28, 29].Figure 5
Fourier transform infrared (FTIR) spectra of sol-gel products, each dried at 100°C for 24 h in air, with Ni/(Ni+Mg) atomic ratio equal to (a) 0.01, (b) 0.05, and (c) 0.10.Figure6 shows the FTIR transmittance spectra of Mg1-xNixO (x=0.01,0.05, and 0.10) produced by decomposition of Ni-doped α-MgC2O4·2H2O at 600°C for 2 h in air. These contain signatures of adsorption and chemisorption of water. The sharp peak centred around 3699 cm−1 indicates the presence of hydroxyl group at the low-coordination sites or defects [5, 28, 29]. The absorption band in the wave number range 3672–3000 cm−1 is quite broad and can be assigned to –OH-stretching mode of adsorbed H2O on the surface of oxide crystallites. The absorption band in the range of 1300–1750 cm−1 is related to hydroxyl groups of molecular water. Since the spectra were not recorded in situ, the products could reabsorb some water from the ambient.Figure 6
Fourier transform infrared (FTIR) spectra ofMg1-xNixO powders, obtained by decomposition of respective oxalates at 600°C for 2 h each in air for x equal to (a) 0.01, (b) 0.05, and (c) 0.10.


### 3.2.2. UV-VIS Absorption

The optical absorption spectra ofMg1-xNixO (x=0.01,0.5,0.1) powders, obtained by decomposition of dried sol-gel product at 600°C for 2 h in air, in the wavelength range of 200–800 nm are shown in Figure 7. The optical absorption of pure MgO prepared similarly has already been presented elsewhere [5]. Table 1 summarises the optical data in terms of peak energy and absorbance. In pure MgO, a magnesium atom donates two electrons from its 3s2-orbitals to 2p-orbitals of oxygen. An energy band gap is thus created between the valence band (oxygen 2p) and conduction band (magnesium, 3s). The known value of energy band gap (Eg) of MgO is about 7.8 eV [5, 27]. A strong absorption band near 202 nm and two other peaks around 296 and 379 nm appear in pure MgO. The former corresponds to (A11g→T1u1) transition from 3P2 state of oxygen (O2−) to 1S0 state of magnesium (Mg2+). The other two peaks at 296 and 379 nm are assigned to A11g→E1 (1s→2px or 2py) and A11g→A11g (1s → 2pz) transitions of oxygen defect centres [5, 30]. With incorporation of Ni2+ ions in MgO, absorption peaks shift slightly, and correspond to improved absorbance  (Table 1, Figure 7). Since no additional band appears, Ni2+ ion is possibly substituting Mg2+ ion in MgO but somehow influencing the absorbance significantly.Table 1
Optical absorption peaks observed inMg1–xNixO nanopowders, prepared by decomposition of dried sol-gel-derived oxalate at 600°C for 2 h each in air for nickel content
(x) = 0, 0.01, 0.05, and 0.10.
No.
x
Peak 1
Peak 2
Peak 3
E (eV)
Abs.
E (eV)
Abs.
E (eV)
Abs.
1*
0
6.13+
0.97
4.20#
0.20
3.27†
0.24
2
0.01
6.13
0.98
4.27
0.27
3.35
0.30
3
0.05
6.20
1.15
4.33
0.36
3.22
0.33
4
0.10
6.10
1.09
4.26
0.45
3.09
0.37
*[5].
+ 1
A
1
g
→
1
T
1
u
(
1
s
→
2
p
x
,
2
p
y
,
or
2
p
z
).
# 1
A
1
g
→
1
E
(
1
s
→
2
p
x
or
2
p
y
).
† 1
A
1
g
→
1
A
1g
(
1
s
→
2
p
z
).Figure 7
Optical absorption spectra ofMg1-xNixO powders, obtained by decomposition of respective oxalates at 600°C for 2 h each in air for x equal to (a) 0.01, (b) 0.05, and (c) 0.10.


### 3.2.3. Photoluminescence (PL) Behaviour

Photoluminescence (PL) spectra ofMg1-xNixO (x=0.01,0.05,0.10) powders, obtained by decomposition of respective oxalates at 1000°C for 2 h in air, with the excitation wavelength of 350 nm are shown in Figure 8. They exhibit a luminescence band centred at 440 nm which becomes broad and shifts slightly towards a higher wavelength (or lower energy) when Ni content (x) increases in MgO matrix. Further, a new emission peak begins to develop near 400 nm and its intensity increases progressively with nickel concentration. This observation suggests changes in the symmetry and vibrational modes around the luminescent centres with nickel doping. Since there is small difference and  ionic radius of Ni2+ (0.69 Å) being smaller than Mg2+ (0.72 Å), the former is possibly substituting the latter in MgO.Figure 8
Photoluminescence (PL) spectra of theMg1-xNixO powders for x equal to (a) 0.01, (b) 0.05, and (c) 0.10.Pure MgO sample prepared similarly exhibits two emission peaks (strong around 440 nm and weak at 395 nm) with the excitation wavelength of 350 nm and are assigned toB21u→A1g and T21u→A21g transitions, respectively [8]. Moreover, their origin lies with the existence of F22+ (or F+ dimers) and F+-colour centres, respectively, F+ being oxygen vacancy retaining one electron [8]. This fact in conjunction with the above results indicates that partial substitution of Mg2+ by Ni2+ ions causes decrease of F+ dimers with simultaneous increase of F+-defect centres in MgO. The process can occur in two ways, namely, F+ dimer either splits into two F+ centres or converts into one F+ centre with transfer of extra electron rendering Ni2+→Ni1+conversion. It may be mentioned that Ni2+ ion has an empty (eg) low-spin orbital.Photoluminescence studies of pure MgO nanocrystals with excitation wavelength of 273 nm have revealed a broad emission band centred around 350 nm arising due to oxygen vacancies [13, 30]. In Dy3+-doped MgO, emission peaks appear at 480 nm and 575 nm due to 4F9/2 − 6H15/2 and 4F9/2 − 6H13/2 transitions of dysprosium [18]. In fact, Dy3+-ions encounter difficulty in substitution because of their large size (ionic radii being 0.91 Å against 0.72 Å of Mg2) and therefore lie essentially on the surface or in the grain boundaries giving its own PL emission at 575 nm. On the other hand, Ni2+ ions can assume Mg2+ sites easily and influence the nature of emission. As a consequence, the peak at 440 nm diminishes and that near 400 nm rises due to decrease in F22+ centres (or dimers) and formation of additional F+ centres occurring in MgO.Upon substitution, Ni2+ ion occupies an octahedral void in MgO and so is coordinated with six oxygen ions. The energy level diagram of Ni2+ (3d8) ion suggests three major thermoradiative energy transitions, 1A1→1E (1117 nm, 1.110 eV), 3T2→3A2 (1256 nm, 0.987 eV), and 1T2→1E (1414 nm, 0.877 eV) at 1300–1400°C. Thus, Ni-doped MgO may also serve as a potential emitter for thermophotovoltaic (TPV) generators [20, 21]. Work is in progress in this direction.


## 3.2.1. Infrared Absorption

The FTIR spectra of sol-gel-derived oxalate samples of Ni/(Ni+Mg) atomic ratios (x) 0.01, 0.05, and 0.10 are shown in Figure 5. The broad absorption band around 3408 cm−1 is in fact composed of several peaks in the wave number range of 3100–3700 cm−1. These correspond to the –OH group stretching vibrations and provide evidence for the presence of chemically bound water. The deformational mode of water usually seen around 1650 cm−1 is, however, masked by the doublet at 1667 cm−1. The other sharp absorption peaks at 1373 and 1325 cm−1 are assigned to νs (C–O) and δ  (OC=O) modes. While weak band at 696 cm−1 is attributed to bending mode of O=C=O and/or liberation of water, a peak at 501 cm−1 is assigned to ν (Mg–O) + ν (C–C) modes [5, 28, 29].Figure 5
Fourier transform infrared (FTIR) spectra of sol-gel products, each dried at 100°C for 24 h in air, with Ni/(Ni+Mg) atomic ratio equal to (a) 0.01, (b) 0.05, and (c) 0.10.Figure6 shows the FTIR transmittance spectra of Mg1-xNixO (x=0.01,0.05, and 0.10) produced by decomposition of Ni-doped α-MgC2O4·2H2O at 600°C for 2 h in air. These contain signatures of adsorption and chemisorption of water. The sharp peak centred around 3699 cm−1 indicates the presence of hydroxyl group at the low-coordination sites or defects [5, 28, 29]. The absorption band in the wave number range 3672–3000 cm−1 is quite broad and can be assigned to –OH-stretching mode of adsorbed H2O on the surface of oxide crystallites. The absorption band in the range of 1300–1750 cm−1 is related to hydroxyl groups of molecular water. Since the spectra were not recorded in situ, the products could reabsorb some water from the ambient.Figure 6
Fourier transform infrared (FTIR) spectra ofMg1-xNixO powders, obtained by decomposition of respective oxalates at 600°C for 2 h each in air for x equal to (a) 0.01, (b) 0.05, and (c) 0.10.


## 3.2.2. UV-VIS Absorption

The optical absorption spectra ofMg1-xNixO (x=0.01,0.5,0.1) powders, obtained by decomposition of dried sol-gel product at 600°C for 2 h in air, in the wavelength range of 200–800 nm are shown in Figure 7. The optical absorption of pure MgO prepared similarly has already been presented elsewhere [5]. Table 1 summarises the optical data in terms of peak energy and absorbance. In pure MgO, a magnesium atom donates two electrons from its 3s2-orbitals to 2p-orbitals of oxygen. An energy band gap is thus created between the valence band (oxygen 2p) and conduction band (magnesium, 3s). The known value of energy band gap (Eg) of MgO is about 7.8 eV [5, 27]. A strong absorption band near 202 nm and two other peaks around 296 and 379 nm appear in pure MgO. The former corresponds to (A11g→T1u1) transition from 3P2 state of oxygen (O2−) to 1S0 state of magnesium (Mg2+). The other two peaks at 296 and 379 nm are assigned to A11g→E1 (1s→2px or 2py) and A11g→A11g (1s → 2pz) transitions of oxygen defect centres [5, 30]. With incorporation of Ni2+ ions in MgO, absorption peaks shift slightly, and correspond to improved absorbance  (Table 1, Figure 7). Since no additional band appears, Ni2+ ion is possibly substituting Mg2+ ion in MgO but somehow influencing the absorbance significantly.Table 1
Optical absorption peaks observed inMg1–xNixO nanopowders, prepared by decomposition of dried sol-gel-derived oxalate at 600°C for 2 h each in air for nickel content
(x) = 0, 0.01, 0.05, and 0.10.
No.
x
Peak 1
Peak 2
Peak 3
E (eV)
Abs.
E (eV)
Abs.
E (eV)
Abs.
1*
0
6.13+
0.97
4.20#
0.20
3.27†
0.24
2
0.01
6.13
0.98
4.27
0.27
3.35
0.30
3
0.05
6.20
1.15
4.33
0.36
3.22
0.33
4
0.10
6.10
1.09
4.26
0.45
3.09
0.37
*[5].
+ 1
A
1
g
→
1
T
1
u
(
1
s
→
2
p
x
,
2
p
y
,
or
2
p
z
).
# 1
A
1
g
→
1
E
(
1
s
→
2
p
x
or
2
p
y
).
† 1
A
1
g
→
1
A
1g
(
1
s
→
2
p
z
).Figure 7
Optical absorption spectra ofMg1-xNixO powders, obtained by decomposition of respective oxalates at 600°C for 2 h each in air for x equal to (a) 0.01, (b) 0.05, and (c) 0.10.


## 3.2.3. Photoluminescence (PL) Behaviour

Photoluminescence (PL) spectra ofMg1-xNixO (x=0.01,0.05,0.10) powders, obtained by decomposition of respective oxalates at 1000°C for 2 h in air, with the excitation wavelength of 350 nm are shown in Figure 8. They exhibit a luminescence band centred at 440 nm which becomes broad and shifts slightly towards a higher wavelength (or lower energy) when Ni content (x) increases in MgO matrix. Further, a new emission peak begins to develop near 400 nm and its intensity increases progressively with nickel concentration. This observation suggests changes in the symmetry and vibrational modes around the luminescent centres with nickel doping. Since there is small difference and  ionic radius of Ni2+ (0.69 Å) being smaller than Mg2+ (0.72 Å), the former is possibly substituting the latter in MgO.Figure 8
Photoluminescence (PL) spectra of theMg1-xNixO powders for x equal to (a) 0.01, (b) 0.05, and (c) 0.10.Pure MgO sample prepared similarly exhibits two emission peaks (strong around 440 nm and weak at 395 nm) with the excitation wavelength of 350 nm and are assigned toB21u→A1g and T21u→A21g transitions, respectively [8]. Moreover, their origin lies with the existence of F22+ (or F+ dimers) and F+-colour centres, respectively, F+ being oxygen vacancy retaining one electron [8]. This fact in conjunction with the above results indicates that partial substitution of Mg2+ by Ni2+ ions causes decrease of F+ dimers with simultaneous increase of F+-defect centres in MgO. The process can occur in two ways, namely, F+ dimer either splits into two F+ centres or converts into one F+ centre with transfer of extra electron rendering Ni2+→Ni1+conversion. It may be mentioned that Ni2+ ion has an empty (eg) low-spin orbital.Photoluminescence studies of pure MgO nanocrystals with excitation wavelength of 273 nm have revealed a broad emission band centred around 350 nm arising due to oxygen vacancies [13, 30]. In Dy3+-doped MgO, emission peaks appear at 480 nm and 575 nm due to 4F9/2 − 6H15/2 and 4F9/2 − 6H13/2 transitions of dysprosium [18]. In fact, Dy3+-ions encounter difficulty in substitution because of their large size (ionic radii being 0.91 Å against 0.72 Å of Mg2) and therefore lie essentially on the surface or in the grain boundaries giving its own PL emission at 575 nm. On the other hand, Ni2+ ions can assume Mg2+ sites easily and influence the nature of emission. As a consequence, the peak at 440 nm diminishes and that near 400 nm rises due to decrease in F22+ centres (or dimers) and formation of additional F+ centres occurring in MgO.Upon substitution, Ni2+ ion occupies an octahedral void in MgO and so is coordinated with six oxygen ions. The energy level diagram of Ni2+ (3d8) ion suggests three major thermoradiative energy transitions, 1A1→1E (1117 nm, 1.110 eV), 3T2→3A2 (1256 nm, 0.987 eV), and 1T2→1E (1414 nm, 0.877 eV) at 1300–1400°C. Thus, Ni-doped MgO may also serve as a potential emitter for thermophotovoltaic (TPV) generators [20, 21]. Work is in progress in this direction.


## 4. Conclusions

Mg
1
-
x
Ni
x
O nanopowders synthesized by decomposition of sol-gel-derived oxalate in air at 600°C or above for 2 h exhibit (i) an f.c.c. (NaCl-type) structure with a typical lattice parameter of 4.228(2) Å at x=0.01, (ii) three optical absorption bands at 6.13 eV, 4.27 eV, and 3.35 eV corresponding to A11g→T1u1, A11g→E1, and A11g→A11g transitions, and (iii) signature of water affinity with a sharp peak at 3699 cm−1 and bands in the range 3672–3000 cm−1 and 1300–1750 cm−1 in the FTIR spectra. Their photoluminescence characteristics with the excitation wavelength of 350 nm depend on the nickel content and are altered in terms of emission (i) reduction at 440 nm due to decrease in F22+ centres and (ii) enhancement near 400 nm because of emergence of additional F+ centres. Ni-doped MgO may serve as emitter in thermophotovoltaic generators too.



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*Source: 865373-2012-11-20.xml*