# Structural, Optical, and Compactness Characteristics of NanocrystallineCaNb

Authors: K. C. Mathai; S. Vidya; Annamma John; Sam Solomon; J. K. Thomas
Journal: Advances in Condensed Matter Physics
 (2014)

---

## Abstract

Nanoparticles of calcium metaniobate compound are prepared by an autoigniting combustion technique and its structural, optical, and dielectric properties are investigated. The X-ray diffraction, Fourier-transform Raman, and infrared studies reveal that calcium metaniobate possesses phase pure orthorhombic columbite structure with space group of Pbcn. The average particle size of the as-prepared nanoparticles obtained from both the Scherrer formula and transmission electron microscopy is ~37 nm. The optical band gap calculated from Tauc's Plot is 3.25 eV. Photoluminescence studies reveal that Calcium metaniobate can be used as an idealphotoluminarmaterial. The powders are pelletised and sintered at an optimized temperature of1350
∘
C in a short duration of two hours, yielding a high density. The morphology of the sintered pellet is further examined using scanning electron microscopy. The dielectric constant and loss factor values measured at 5 MHz for a well-sintered Calcium metaniobate pellet are found to be 27.6 and 5.3
×
10
−
4 respectively, at room temperature.


---

## Body

## 1. Introduction

Calcium metaniobate (CaNb2O6) crystallizes with orthorhombic columbite structure in the space group of Pbcn(60) and is a strong source of coherent light which can be useful in applications of holography [1]. CaNb2O6 crystal possesses a low-symmetry crystal structure and the Ca and Nb cations are at the centre of the octahedra surrounded by six oxygen atoms in the   CaNb2O6 columbite structure. The CaO6 and NbO6 octahedra form independent zigzag chains by sharing edges and the chains are connected by sharing corners in the order of CaO6 chain-NbO6 chain-NbO6 chain [2, 3]. CaNb2O6 has good mechanical, dielectric, and thermal properties like thermal conductivity, specific heat, and thermal coefficient of expansion making it suitable for laser crystal host, substrates for electronic circuits, and so forth [1, 3]. The photocatalytic activity of CaNb2O6 is studied by a number of researchers and Cho et al. reported its enhanced photocatalytic activity for producing H2 from pure water under UV irradiation [4–7]. CaNb2O6 also exhibits strong blue luminescence emission under UV light irradiation at 300 K. CaNb2O6 also possesses interesting properties, namely, piezoelectricity, pyroelectricity, and electrooptic and nonlinear optical activity [8–11]. The compacted calciummetaniobate (CaNb2O6) is a good dielectric material for microwave dielectric applications [12–14]. CaNb2O6, a subcomponent of the complex perovskite family A(B
1
/
3
′
B
2
/
3
′′)O3 prepared by the conventional route, has been studied for its microwave dielectric properties [15–17]. Generally, the relative band positions, optical band gaps, and so forth, in niobate compounds, are affected by the characteristic of their crystal structure, octahedral distortion, and the ionic size of cations [7]. The various synthesis techniques employed for the preparation of CaNb2O6 are conventional solid state route, hydrothermal synthesis, solvothermal process, and sol-gel technique [6, 7, 17, 18].In the present work, we have synthesized calcium metaniobate (CaNb2O6) nanopowder using an autoigniting combustion technique, and its structural, optical, and dielectric properties are investigated.


## 2. Experimental

### 2.1. Synthesis Procedure

In the present autoigniting combustion synthesis, aqueous solution containing ions of Ca and Nb is prepared by dissolving stoichiometric amount of high purity Ca(NO3)2 (99%, CDH, India) in double distilled water and NbCl5 (99.9%, Alfa Aesar) in hot oxalic acid. Citric acid was added as a complexing agent maintaining the citric acid to the cation ratio at unity. Amount of citric acid was calculated based on total valence of the oxidizing and the reducing agents for maximum release of energy during combustion [16, 19]. Appropriate amount of urea, as fuel, and nitric acid, as oxidizer, was added to the precursor to obtain a clear viscous solution. The solution which is acidic in nature, containing the precursor mixture, was then heated using a hot plate at ~250°C in a ventilated fume hood. The solution boils on heating and undergoes dehydration accompanied by foam. The foam gets ignited by itself on persistent heating giving voluminous and fluffy product of combustion. Thus the obtained as-prepared powder was taken for further characterizations.


### 2.2. Characterization Technique

The crystal structure of the prepared particle was determined by X-ray technique using PHILIPS XPERT-PRO diffractometer with nickel filtered CuKα radiation of wavelength 1.5406 Å
´. The Fourier transform-Raman spectrum was carried out at room temperature in the wave number range 50–1200 cm−1 using Bruker-RFS/100S spectrometer at a power level of 150 mW and at a resolution of 4 cm−1. The sample was excited with an Nd:YAG laser lasing at 1064 nm, and the scattered radiations were detected using Ge detector. The infrared (IR) spectra of the sample were recorded in the range 400–4000 cm−1 using a Thermo-Nicolet Avatar 370 FTIR Spectrometer using KBr pellet method. Particulate properties of the combustion product were examined using transmission electron microscopy (TEM Hitachi H-600, Japan). The photoluminescence (PL) spectrum of the sample was measured using Flurolog@-3 Spectrofluorometer. The photons from the source were filtered by an excitation spectrometer. The monochromatic radiation was then allowed to fall on the disc samples and the resulting radiation was filtered by an emission spectrometer and then fed to a photomultiplier detector. The optical measurements of the nanopowder were carried out at room temperature using a Cary 100 BIO UV-Vis spectrophotometer in the wavelength range 200–700 nm.To study the sinterability of the nanoparticles obtained by the present combustion method, the as-prepared CaNb2O6 nanoparticles were mixed with 5% polyvinyl alcohol and pressed in the form of cylindrical pellet of 12 mm diameter and ~2 mm thickness at a pressure about 350 MPa using a hydraulic press. The sintering temperature of the pellet was optimized at 1350°C for 2 hours after conducting many trials. The surface morphology of the sintered sample was examined using scanning electron microscopy (SEM, Model-JEOL JSM 6390LV). For low frequency dielectric studies the pellet was made in the form of a disc capacitor with the specimen as the dielectric medium. Both the flat surfaces of the sintered pellet were polished and then electroded by applying silver paste. The capacitance of the sample was measured using an LCR meter (Hioki-3532-50LCR HiTester) in the frequency range 100 Hz to 5 MHz at room temperature.


## 2.1. Synthesis Procedure

In the present autoigniting combustion synthesis, aqueous solution containing ions of Ca and Nb is prepared by dissolving stoichiometric amount of high purity Ca(NO3)2 (99%, CDH, India) in double distilled water and NbCl5 (99.9%, Alfa Aesar) in hot oxalic acid. Citric acid was added as a complexing agent maintaining the citric acid to the cation ratio at unity. Amount of citric acid was calculated based on total valence of the oxidizing and the reducing agents for maximum release of energy during combustion [16, 19]. Appropriate amount of urea, as fuel, and nitric acid, as oxidizer, was added to the precursor to obtain a clear viscous solution. The solution which is acidic in nature, containing the precursor mixture, was then heated using a hot plate at ~250°C in a ventilated fume hood. The solution boils on heating and undergoes dehydration accompanied by foam. The foam gets ignited by itself on persistent heating giving voluminous and fluffy product of combustion. Thus the obtained as-prepared powder was taken for further characterizations.


## 2.2. Characterization Technique

The crystal structure of the prepared particle was determined by X-ray technique using PHILIPS XPERT-PRO diffractometer with nickel filtered CuKα radiation of wavelength 1.5406 Å
´. The Fourier transform-Raman spectrum was carried out at room temperature in the wave number range 50–1200 cm−1 using Bruker-RFS/100S spectrometer at a power level of 150 mW and at a resolution of 4 cm−1. The sample was excited with an Nd:YAG laser lasing at 1064 nm, and the scattered radiations were detected using Ge detector. The infrared (IR) spectra of the sample were recorded in the range 400–4000 cm−1 using a Thermo-Nicolet Avatar 370 FTIR Spectrometer using KBr pellet method. Particulate properties of the combustion product were examined using transmission electron microscopy (TEM Hitachi H-600, Japan). The photoluminescence (PL) spectrum of the sample was measured using Flurolog@-3 Spectrofluorometer. The photons from the source were filtered by an excitation spectrometer. The monochromatic radiation was then allowed to fall on the disc samples and the resulting radiation was filtered by an emission spectrometer and then fed to a photomultiplier detector. The optical measurements of the nanopowder were carried out at room temperature using a Cary 100 BIO UV-Vis spectrophotometer in the wavelength range 200–700 nm.To study the sinterability of the nanoparticles obtained by the present combustion method, the as-prepared CaNb2O6 nanoparticles were mixed with 5% polyvinyl alcohol and pressed in the form of cylindrical pellet of 12 mm diameter and ~2 mm thickness at a pressure about 350 MPa using a hydraulic press. The sintering temperature of the pellet was optimized at 1350°C for 2 hours after conducting many trials. The surface morphology of the sintered sample was examined using scanning electron microscopy (SEM, Model-JEOL JSM 6390LV). For low frequency dielectric studies the pellet was made in the form of a disc capacitor with the specimen as the dielectric medium. Both the flat surfaces of the sintered pellet were polished and then electroded by applying silver paste. The capacitance of the sample was measured using an LCR meter (Hioki-3532-50LCR HiTester) in the frequency range 100 Hz to 5 MHz at room temperature.


## 3. Results and Discussion

### 3.1. Structural Characterizations

Figure1 shows the XRD patterns of as-prepared calcium metaniobate nanopowder. All the peaks are indexed for orthorhombic structure and agree well with reported value (JCPDS 391392). The calculated lattice constants are a
=
5.727 Å, b
=
14.807 Å, and c
=
5.239 Å, which indicate that the formation of CaNb2O6 phase is complete during the combustion process itself. The average crystallite size calculated from full width half maximum (FWHM) using the Scherrer formula is ~37 nm.Figure 1
XRD patterns of as-prepared CaNb2O6.


### 3.2. FT-Raman and Infrared Spectroscopy of CaNb2O6

The X-ray diffraction study revealed that the as-prepared nanocrystalline CaNb2O6 is orthorhombic structure with space group Pbcn.  To investigate more on the structural details of CaNb2O6, FTIR and Raman spectra of the sample are also recorded and are shown in Figures 2 and 3, respectively.Figure 2
FT-Raman spectrum of the as-prepared CaNb2O6 nanopowder.Figure 3
FT-IR spectrum of the as-prepared CaNb2O6 nanopowder.The spectral data of the Raman and IR spectra and the band assignments are given in Table1. The Raman spectrum over the range 1000–100 cm−1 is characterized by the Nb–O stretching vibrations. As expected the ν
1
(
A
g
) mode which is attributed to the terminal Nb–O stretching vibration is observed as a sharp highly intense band at 904 cm−1 [20, 21]. The bridge Nb–O stretching vibration occurs in the range 700–500 cm−1 and the chain Nb–O stretching vibration below 500 cm−1. The bands due to ν
2 mode of vibration of the A
g, B
1
g, B
2
g, and B
3
g symmetries appear unresolved and are observed as an intense broad band extending from about 800 to 610 cm−1 with the peak at 695 cm−1. The weak band at 578 cm−1 may be a combination band due to combination like ν
6
(
A
g
)
+
ν
7
(
A
g
) or ν
6
(
B
2
g
)
+
ν
7
(
B
2
g
). The O–Nb–O bending vibrations occur in the range 450–100 cm−1. The Ca–O stretching and the vibrations involving the chain bonds and Nb–Nb bonds occur towards the lower wavenumbers of this range. The lowest frequency band at 75 cm−1 of appreciable intensity is due to the lattice vibrations.Table 1
Raman and IR spectral data of CaNb2O6 and their band assignment relative intensities. v: very, s: strong, m: medium, w: weak, sh: shoulder, and br: broad.
Raman (cm−1)
Band assignments
IR (cm−1)
Band assignments
904 vvs
ν
1
(
A
g
)
846 w
ν
1
(
B
1
g
)
867 vs
ν
1
(
B
2
u
)
695 vsbr
ν
2
(
A
g
), ν
2
(
B
1
g
),
ν
2
(
B
2
g
), ν
2
(
B
3
g
),
805 s
ν
3
(
B
1
u
)
+
ν
7
(
B
1
u
)
626 sh
ν
3
(
B
3
g
)
747 s
ν
2
(
B
2
u
)
597 vvw
ν
3
(
B
1
g
)
578 vw
ν
6
(
A
g
)
+
ν
7
(
A
g
)/
ν
6
(
B
2
g
)
+
ν
7
(
B
2
g
)
538 s
ν
3
(
A
g
)
550 vsbr
ν
3
(
B
1
u
), ν
3
(
B
2
u
),
ν
3
(
B
3
u
)
493 m
ν
4
(
B
1
g
), ν
3
(
B
2
g
)
497 m
ν
4
(
B
1
u
), ν
4
(
B
3
u
)
458 vvw
ν
4
(
B
2
g
)
427 vw
ν
5
(
B
1
g
)
382 s
ν
5
(
A
g
), ν
5
(
B
2
g
)
345 vw
ν
7
(
B
1
g
)
313 vw
ν
6
(
B
2
g
)
289 s
ν
6
(
A
g
), ν
7
(
A
g
), ν
8
(
B
1
g
)
262 w
ν
9
(
B
1
g
), ν
7
(
B
2
g
)
241 s
ν
8
(
A
g
)
221 vw
ν
9
(
A
g
), ν
9
(
B
2
g
)
194 m
ν
10
(
A
g
)
163 w
ν
12
(
B
1
g
)
136 m
ν
11
(
A
g
), ν
11
(
B
3
g
)
107 vw
ν
12
(
B
2
g
)
75 s
Lattice vibrationIn the IR-spectrum, intense absorption is observed in the range 900–400 cm−1. The band at 867 cm−1 is due to the ν
1
(
B
2
u
) mode of vibration and that at 747 cm−1 is due to the ν
2
(
B
2
u
) mode. The intense band at 550 cm−1 is broadened with shoulders on either side. The broadening may be due to the overlapping of the ν
3 mode of vibration of B
1
u, B
2
u, and B
3
u symmetries. The ν
4
(
B
1
u
) and ν
4
(
B
3
u
) modes are observed as a medium intense absorption at 497 cm−1. The band at 805 cm−1 may be due to the combination ν
3
(
B
1
u
)
+
ν
7
(
B
1
u
).Thus the factors like Nb–O stretching, O–Nb–O bending, Ca–O stretching, and the vibrations involving chain bonds and the broadening of the peaks indicate a slightly distorted      (NbO6 octahedra) crystal structure.


### 3.3. TEM Studies

TEM image of the CaNb2O6 samples is shown in Figure 4, and inset shows the corresponding SAED pattern. TEM image of the as-prepared sample showed that the nanoparticles are of submicron size 24–50 nm. The particles are of regular cuboidal shape with average size of nearly 37 nm. The selected area electron diffraction (SAED) pattern indicates the polycrystalline nature of the crystallites. The spotty nature is due to the finer crystallites having related orientations agglomerated together resulting in a limited set of orientations.Figure 4
TEM image of as-prepared CaNb2O6 nanopowder and its SAED pattern inset.


### 3.4. Optical Studies

The UV absorption spectra of the prepared nanoparticles of CaNb2O6 samples measured using a Cary 100 BIO UV-Vis spectrophotometer in the range 200–700 nm are shown in Figure 5.Figure 5
UV-Vis absorption spectrum of CaNb2O6 nanopowder.In semiconductors, the absorption coefficient near the fundamental edge depends on photon energy. This absorption dependence on photon energy is expressed by Tauc’s equation [10]. According to Tauc’s relation, the absorption coefficient, for direct band gap material, is given by
(1)
(
α
h
ν
)
=
B
[
h
ν
-
E
g
]
m
,
where B is the absorption coefficient, E
g is the optical band gap energy, h is Planck’s constant, νis the frequency of incident photon, and m is an index which depends on the nature of electronic transition responsible for the optical absorption. Values of m for allowed direct and indirect transitions are 1/2 and 2, respectively. Optical transitions of the samples under study are indirect one. The indirect optical energy gap can be obtained from the intercept of the resulting linear region with the energy axis at (
α
h
ν
)
2
=
0. Figure 6 shows the Tauc’s plot of the optical absorption spectrum measured at room temperature for calcium metaniobate nanopowder. Thus the determined band gap of calcium metaniobate is 3.25 eV. The absorption spectra indicate that the sample absorbs heavily in UV region and moderately in the visible region. Such materials find tremendous applications in UV filters and sensors.Figure 6
Tauc’s plot of the optical absorption spectrum of CaNb2O6 nanopowder.


### 3.5. Photoluminescence Study

The photoluminescence activity of the samples was investigated by recording the PL emission spectra of the as-prepared samples. The obtained PL spectra at the excitation wavelength of 350 nm are shown in Figure7. The sample shows good luminescent property in the visible region. The transmission responsible for each emission is identified on the basis of the data by Payling and Larkins [22]. For CaNb2O6, the intense peak in the blue region at 442.5 nm corresponds to 3
P
0
0
-
3
D
1 of CaI. The peak at 485.6 nm corresponds to 4
S
1.5
0
-
4
D
1.5 transition of OII. The peak at 528 nm is attributed to 3
D
1
-
1
P
1
0 transition of NbI. The strong emission lines of the sample at specific wavelength make it useful in optoelectronic applications.Figure 7
PL emission spectra of CaNb2O6.


### 3.6. Sintering and Dielectric Properties

For the sintering behavior, the CaNb2O6 nanopowder was compressed as cylindrical discs and was sintered at 1350°C for 2 hours at a heating rate of 5°C/minute. The density of the sintered sample was calculated by “Archimedes” method and obtained >96%. The high density derived through the present study may be attributed to enhanced kinetics due to the small degree of agglomeration and ultrafine nature of the powder.The SEM image of the sample given in Figure8 shows the compactness of the sintered pellet. It is evident from the SEM that the sample achieved high densification with little porosity. From the SEM pattern, long rectangular sheet like patterns can be seen with their size in the micrometer range. Thus heat treatment resulted in grain growth up to several micrometers. The EDAX pattern shows that all the elements such as calcium, niobium, and oxygen are present in the sample in the same stoichiometric concentrations and are shown in Figure 9.Figure 8
SEM micrograph of CaNb2O6.Figure 9
EDAX pattern of CaNb2O6.The dielectric constantε
r and loss factor tan
δ values of the sintered pellets were studied in the frequency range 100 Hz to 5 MHz at room temperature with silver electrodes on both sides of the circular disc. Figure 10 shows variation of ε
r and tan
δ at room temperature with the frequency. The obtained dielectric constant ε
r and loss factor tan
δ values of the CaNb2O6 pellets at 5 MHz were 27.6 and 5.3
×
10
-
4, respectively. The values of dielectric constant and low loss factor indicate the suitability of the sample as a candidate for electronic and dielectric device applications.Figure 10
Variation ofε
r and tan
δ with the frequency.


## 3.1. Structural Characterizations

Figure1 shows the XRD patterns of as-prepared calcium metaniobate nanopowder. All the peaks are indexed for orthorhombic structure and agree well with reported value (JCPDS 391392). The calculated lattice constants are a
=
5.727 Å, b
=
14.807 Å, and c
=
5.239 Å, which indicate that the formation of CaNb2O6 phase is complete during the combustion process itself. The average crystallite size calculated from full width half maximum (FWHM) using the Scherrer formula is ~37 nm.Figure 1
XRD patterns of as-prepared CaNb2O6.


## 3.2. FT-Raman and Infrared Spectroscopy of CaNb2O6

The X-ray diffraction study revealed that the as-prepared nanocrystalline CaNb2O6 is orthorhombic structure with space group Pbcn.  To investigate more on the structural details of CaNb2O6, FTIR and Raman spectra of the sample are also recorded and are shown in Figures 2 and 3, respectively.Figure 2
FT-Raman spectrum of the as-prepared CaNb2O6 nanopowder.Figure 3
FT-IR spectrum of the as-prepared CaNb2O6 nanopowder.The spectral data of the Raman and IR spectra and the band assignments are given in Table1. The Raman spectrum over the range 1000–100 cm−1 is characterized by the Nb–O stretching vibrations. As expected the ν
1
(
A
g
) mode which is attributed to the terminal Nb–O stretching vibration is observed as a sharp highly intense band at 904 cm−1 [20, 21]. The bridge Nb–O stretching vibration occurs in the range 700–500 cm−1 and the chain Nb–O stretching vibration below 500 cm−1. The bands due to ν
2 mode of vibration of the A
g, B
1
g, B
2
g, and B
3
g symmetries appear unresolved and are observed as an intense broad band extending from about 800 to 610 cm−1 with the peak at 695 cm−1. The weak band at 578 cm−1 may be a combination band due to combination like ν
6
(
A
g
)
+
ν
7
(
A
g
) or ν
6
(
B
2
g
)
+
ν
7
(
B
2
g
). The O–Nb–O bending vibrations occur in the range 450–100 cm−1. The Ca–O stretching and the vibrations involving the chain bonds and Nb–Nb bonds occur towards the lower wavenumbers of this range. The lowest frequency band at 75 cm−1 of appreciable intensity is due to the lattice vibrations.Table 1
Raman and IR spectral data of CaNb2O6 and their band assignment relative intensities. v: very, s: strong, m: medium, w: weak, sh: shoulder, and br: broad.
Raman (cm−1)
Band assignments
IR (cm−1)
Band assignments
904 vvs
ν
1
(
A
g
)
846 w
ν
1
(
B
1
g
)
867 vs
ν
1
(
B
2
u
)
695 vsbr
ν
2
(
A
g
), ν
2
(
B
1
g
),
ν
2
(
B
2
g
), ν
2
(
B
3
g
),
805 s
ν
3
(
B
1
u
)
+
ν
7
(
B
1
u
)
626 sh
ν
3
(
B
3
g
)
747 s
ν
2
(
B
2
u
)
597 vvw
ν
3
(
B
1
g
)
578 vw
ν
6
(
A
g
)
+
ν
7
(
A
g
)/
ν
6
(
B
2
g
)
+
ν
7
(
B
2
g
)
538 s
ν
3
(
A
g
)
550 vsbr
ν
3
(
B
1
u
), ν
3
(
B
2
u
),
ν
3
(
B
3
u
)
493 m
ν
4
(
B
1
g
), ν
3
(
B
2
g
)
497 m
ν
4
(
B
1
u
), ν
4
(
B
3
u
)
458 vvw
ν
4
(
B
2
g
)
427 vw
ν
5
(
B
1
g
)
382 s
ν
5
(
A
g
), ν
5
(
B
2
g
)
345 vw
ν
7
(
B
1
g
)
313 vw
ν
6
(
B
2
g
)
289 s
ν
6
(
A
g
), ν
7
(
A
g
), ν
8
(
B
1
g
)
262 w
ν
9
(
B
1
g
), ν
7
(
B
2
g
)
241 s
ν
8
(
A
g
)
221 vw
ν
9
(
A
g
), ν
9
(
B
2
g
)
194 m
ν
10
(
A
g
)
163 w
ν
12
(
B
1
g
)
136 m
ν
11
(
A
g
), ν
11
(
B
3
g
)
107 vw
ν
12
(
B
2
g
)
75 s
Lattice vibrationIn the IR-spectrum, intense absorption is observed in the range 900–400 cm−1. The band at 867 cm−1 is due to the ν
1
(
B
2
u
) mode of vibration and that at 747 cm−1 is due to the ν
2
(
B
2
u
) mode. The intense band at 550 cm−1 is broadened with shoulders on either side. The broadening may be due to the overlapping of the ν
3 mode of vibration of B
1
u, B
2
u, and B
3
u symmetries. The ν
4
(
B
1
u
) and ν
4
(
B
3
u
) modes are observed as a medium intense absorption at 497 cm−1. The band at 805 cm−1 may be due to the combination ν
3
(
B
1
u
)
+
ν
7
(
B
1
u
).Thus the factors like Nb–O stretching, O–Nb–O bending, Ca–O stretching, and the vibrations involving chain bonds and the broadening of the peaks indicate a slightly distorted      (NbO6 octahedra) crystal structure.


## 3.3. TEM Studies

TEM image of the CaNb2O6 samples is shown in Figure 4, and inset shows the corresponding SAED pattern. TEM image of the as-prepared sample showed that the nanoparticles are of submicron size 24–50 nm. The particles are of regular cuboidal shape with average size of nearly 37 nm. The selected area electron diffraction (SAED) pattern indicates the polycrystalline nature of the crystallites. The spotty nature is due to the finer crystallites having related orientations agglomerated together resulting in a limited set of orientations.Figure 4
TEM image of as-prepared CaNb2O6 nanopowder and its SAED pattern inset.


## 3.4. Optical Studies

The UV absorption spectra of the prepared nanoparticles of CaNb2O6 samples measured using a Cary 100 BIO UV-Vis spectrophotometer in the range 200–700 nm are shown in Figure 5.Figure 5
UV-Vis absorption spectrum of CaNb2O6 nanopowder.In semiconductors, the absorption coefficient near the fundamental edge depends on photon energy. This absorption dependence on photon energy is expressed by Tauc’s equation [10]. According to Tauc’s relation, the absorption coefficient, for direct band gap material, is given by
(1)
(
α
h
ν
)
=
B
[
h
ν
-
E
g
]
m
,
where B is the absorption coefficient, E
g is the optical band gap energy, h is Planck’s constant, νis the frequency of incident photon, and m is an index which depends on the nature of electronic transition responsible for the optical absorption. Values of m for allowed direct and indirect transitions are 1/2 and 2, respectively. Optical transitions of the samples under study are indirect one. The indirect optical energy gap can be obtained from the intercept of the resulting linear region with the energy axis at (
α
h
ν
)
2
=
0. Figure 6 shows the Tauc’s plot of the optical absorption spectrum measured at room temperature for calcium metaniobate nanopowder. Thus the determined band gap of calcium metaniobate is 3.25 eV. The absorption spectra indicate that the sample absorbs heavily in UV region and moderately in the visible region. Such materials find tremendous applications in UV filters and sensors.Figure 6
Tauc’s plot of the optical absorption spectrum of CaNb2O6 nanopowder.


## 3.5. Photoluminescence Study

The photoluminescence activity of the samples was investigated by recording the PL emission spectra of the as-prepared samples. The obtained PL spectra at the excitation wavelength of 350 nm are shown in Figure7. The sample shows good luminescent property in the visible region. The transmission responsible for each emission is identified on the basis of the data by Payling and Larkins [22]. For CaNb2O6, the intense peak in the blue region at 442.5 nm corresponds to 3
P
0
0
-
3
D
1 of CaI. The peak at 485.6 nm corresponds to 4
S
1.5
0
-
4
D
1.5 transition of OII. The peak at 528 nm is attributed to 3
D
1
-
1
P
1
0 transition of NbI. The strong emission lines of the sample at specific wavelength make it useful in optoelectronic applications.Figure 7
PL emission spectra of CaNb2O6.


## 3.6. Sintering and Dielectric Properties

For the sintering behavior, the CaNb2O6 nanopowder was compressed as cylindrical discs and was sintered at 1350°C for 2 hours at a heating rate of 5°C/minute. The density of the sintered sample was calculated by “Archimedes” method and obtained >96%. The high density derived through the present study may be attributed to enhanced kinetics due to the small degree of agglomeration and ultrafine nature of the powder.The SEM image of the sample given in Figure8 shows the compactness of the sintered pellet. It is evident from the SEM that the sample achieved high densification with little porosity. From the SEM pattern, long rectangular sheet like patterns can be seen with their size in the micrometer range. Thus heat treatment resulted in grain growth up to several micrometers. The EDAX pattern shows that all the elements such as calcium, niobium, and oxygen are present in the sample in the same stoichiometric concentrations and are shown in Figure 9.Figure 8
SEM micrograph of CaNb2O6.Figure 9
EDAX pattern of CaNb2O6.The dielectric constantε
r and loss factor tan
δ values of the sintered pellets were studied in the frequency range 100 Hz to 5 MHz at room temperature with silver electrodes on both sides of the circular disc. Figure 10 shows variation of ε
r and tan
δ at room temperature with the frequency. The obtained dielectric constant ε
r and loss factor tan
δ values of the CaNb2O6 pellets at 5 MHz were 27.6 and 5.3
×
10
-
4, respectively. The values of dielectric constant and low loss factor indicate the suitability of the sample as a candidate for electronic and dielectric device applications.Figure 10
Variation ofε
r and tan
δ with the frequency.


## 4. Conclusions

Nanocrystalline semiconducting calcium metaniobate has been synthesized through an autoigniting combustion process. The X-ray diffraction study shows that the as-prepared nanopowder is single phase with orthorhombic structure. FT-Raman and FTIR studies showed that samples possess a distorted orthorhombic perovskite structure. TEM and SAED patterns confirm the nanocrystalline nature of the sample with an average particle size of 37 nm. The average optical band gap determined from Tauc’s plot is 3.25 eV. PL measurements reveal that CaNb2O6 is a good photoluminar material. These nanocrystals were sintered at 1350°C to a high density in a short duration of 2 hours. The SEM image of the sintered sample indicates high densification of the material. The room temperature dielectric constant (ε
r) and loss factor (tan
δ) of the sintered pellet at 5 MHz are ~29 and 5.3
×
10
-
4, respectively, which indicate that the material is suitable for electronic applications.



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*Source: 735878-2014-01-09.xml*