Open access peer-reviewed chapter

Gd2O3: A Luminescent Material

By Raunak Kumar Tamrakar and Kanchan Upadhyay

Submitted: September 23rd 2018Reviewed: March 30th 2020Published: May 19th 2020

DOI: 10.5772/intechopen.92310

Downloaded: 46


Luminescence behavior of the Gd2O3 phosphor is one of the important aspects in the technology of rare earth-based inorganic phosphor materials. The structural and optical behavior of a Gd2O3 nanophosphor will be discussed in detail. Structural characterization of the Gd2O3 was carried out via X-ray diffraction and electron microscopy methods. To detail the photoluminescence behavior, the excitation and emission spectra were recorded and discussed. Thermoluminescence (TL) study and kinetic analysis of the UV- and gamma-irradiated phosphor were also carried out to determine the use of the phosphor for the dosimetric application. Tunned glow peaks were deconvoluted by applying glow curve deconvolution function, and all the trapping parameters were determined.


  • Gd2O3
  • combustion synthesis method
  • XRD
  • SEM
  • TEM
  • thermoluminescence
  • photoluminescence

1. Introduction

These days, rare earth oxide luminescent materials have pulled in incredible consideration because of their size, shape, and phase-dependent luminescent behavior, which make them reasonable for various applications. Among various groups of crystalline materials, oxide crystal is of incredible enthusiasm because of their exceptional optical properties, for example, long fluorescent lifetime, extensive Stokes shift, positive physical and chemical properties, and also great photochemical stability. A few of the rare earth components and their relating oxides are of exceedingly specialized significance and are utilized in basic parts. Rare earth oxides are this sort of cutting edge materials, which are generally utilized as elite luminescent gadgets, magnets, catalyst, and other useful materials, for example, electronic, attractive, atomic, optical, and synergist gadgets [1].

Lanthanide hydroxides and oxides have effectively been examined as a result of their extensive variety of utilizations including dielectric materials for multilayered capacitors, luminescent lights and shows, strong laser gadgets, optoelectronic information stockpiles, and waveguides. Lanthanide-doped oxide nanoparticles are of unique interests as potential materials for a vital new class of nanophosphors. At the point when connected for a fluorescent naming, they present a few focal points, for example, sharp emanation spectra, long-life times, and obstruction against photobleaching in examination with ordinary natural fluorophores and quantum spots [1, 2].

Gadolinium oxide (Gd2O3) is one of the good choices to researchers for luminescence behavior because it has high refractive index (2.3), high optical transparency, great thermal and chemical stability, high dielectric consistent, and low phonon energy among the group of oxide [3, 4, 5, 6]. Due to these positive properties, it displays various applications, for example, oxygen gas sensors, anode materials for sensors, optoelectronic gadgets, high definition TVs, medical imaging, high temperature superconducting materials, phenomenal UV light safeguard, photograph impetus, remedial impacts on malignant growth treatment-improving the impact of radiation on destructive cells while diminishing harm to typical cells, luminescent inks, paint and color sunscreen beautifiers, and luminescent materials [7].

Gadolinium oxide-based nanophosphors are observed to guarantee hopefuls in the field of superior luminescent gadgets, catalysis, and other practical gadgets dependent on their great electronic, optical, and physico-concoction reactions emerging from 4f electrons. Of course, every one of these properties could be to a great extent affected by their synthetic synthesis, precious stone structure, shape, and dimensionality. In this way, high surface region nanomaterial, which has a bigger part of deformity locales per unit zone, ought to be of enthusiasm as adsorbents in ecological remediation forms. Cost of amalgamation, effortlessness, and morphological attributes of arranged phosphor are vital parameters for their utilization in the business applications as it is basic that a self-spreading ignition course offers the best decision for the blend of Gd2O3 powder [2, 7].

Nanoparticles arranged by combustion synthesis have size of ~10 nm; such methodologies include the utilization of organic fuels such as urea, glycine, and so forth to start deterioration response of precursor metal salt at high temperature. The higher reactivity of littler size Gd2O3 particles is not simply because of the vast explicit surface region, yet in addition, because of the high concentration of low planned destinations and basic imperfections on their surface. Because of these benefits, these are sought after for different innovative applications including optoelectronic gadgets, top quality TVs, organic imaging and labeling, MRI, luminescent paints and inks for security codes, and so forth [8].

In the present work, combustion synthesis has been used for preparation of gadolinium oxide by utilizing glycerin and urea as a fuel. The union and portrayal of gadolinium oxide through various strategies have pulled in impressive consideration. The fuel and metal nitrate get deteriorated and give combustible gases, for example, NH3, CO2, and NO2. At the point when the arrangement achieves a point of sudden ignition, it starts consuming and turns into a consuming strong. The ignition proceeds until the point that all the combustible substances have wore out, and it ends up being a free substance with voids and pores framed by the getting away gases amid the burning response. The entire procedure takes just a couple of minutes to yield powder of oxide. The auxiliary and optical portrayals of the incorporated powders were completed utilizing X-beam powder diffractometer. Checking electron microscopy (SEM) was utilized to show the development of crystallites, and TEM was utilized for molecular measure affirmation. Fourier Transform Infrared Spectroscopy (FTIR) range of Gd2O3 nanopowder was acquired by utilizing FTIR spectrophotometer (Model; MIR 8300TM) with KBr blend in the pellet shape. The Raman and X-ray photoelectron spectroscopic studies of the prepared phosphor were also carried out.

2. Materials and methods

2.1 Synthesis

Phosphor was synthesized by combustion synthesis method. Gadolinium nitrate was used as precursor solution and urea or glycine as fuel. Aqueous solution of gadolinium nitrate was prepared by dissolving suitable amount of precursor into double distilled water followed by the addition of fuel. The mixture was kept in a magnetic stirrer at 60°C and stirred for 4 h, and a transparent gel was obtained. Gel was transferred into alumina crucible and kept in a preheated furnace at 600°C. The gel mixture undergoes dehydration followed by spontaneous combustion to form Gd2O3 powder [1, 2]. The resulting brownish powder was heated until a controlled explosion took place yielding a very fine, white powder. Since the reaction is so rapid, the crystal growth will be highly restrained (Figures 1 and 2).

Figure 1.

Flow chart of synthesis of Gd2O3 with urea (reproduced from [1]).

Figure 2.

Flow chart of synthesis of Gd2O3 with glycerin (reproduced from [2]).

2.2 Material characterization

The crystallinity of the phosphor was checked by X-ray diffraction estimation. The X-ray powder diffraction information was gathered by utilizing Bruker D8 Advanced X-ray diffractometer using Cu Kα radiation. The X-beams were created utilizing a fixed cylinder, and the wave length of X-beam was 0.154 nm. The X-rays were identified utilizing a quick checking indicator dependent on silicon strip technology (Bruker Lynx Eye finder). The surface morphology of the phosphors was detected by field emission electron microscopy (FESEM) JSM-7600F. Energy dispersive X-ray examination (EDX) was utilized for compositional investigation of the phosphor. Crystal size of arranged phosphor was determined by Transmission Electron Microscopy (TEM) utilizing Philips CM-200. Raman spectra were recorded by Jobin-Yvon, France, Ramnor HG-2S Spectrometer with Ar-Laser with 4 W control having goals of 0.5 cm−1 and wave number exactness of 1 cm−1 over 5000 cm−1. XPS investigation was performed in a VG instrument with a CLAM2 analyzer and a twin Mg/Al anode. The weight pressure in the investigation chamber was roughly 9 × 10−10 mbar. The estimations were done with unmonochromated Al Kα photons (1486.6 eV). The intensity of the X-ray source was kept steady at 300 W.

3. Result and discussion

3.1 XRD result

The XRD pattern of the Gd2O3 sample is shown in Figure 3. The diffraction patterns are well matched with standard JCPDS card no. 43-1015, indicating that the sample of Gd2O3 phosphor is in the pure monoclinic phase. The particle size was calculated by the Scherer formula [7]

Figure 3.

XRD patterns of Gd2O3: (A) glycerin fuel and (B) urea fuel.


where D is the volume weighted crystallite size, k is the shape factor (0.9), λ is the wavelength of Cu Kα1 radiation, β hkl is the instrumental corrected integral breadth of the reflection (in radians) located at 2θ, and θ is the angle of reflection (in degrees) utilized to relate the crystallite size to the line broadening. The average crystallite size of Gd2O3 nanoparticles was found to be in the range of 8–10 nm for both the fuels. No impurity peaks or other possible phases of Gd2O3 were observed. Further, the strong and sharp diffraction peaks confirm the high crystallinity of the products.

3.2 Surface morphology

The scanning electron microscopy (SEM) was utilized as a focused ray of high energy electrons to produce an assortment of signs at the crystalline surface. The signs that get from electron and sample interaction uncover data about the example including outer morphology, elemental composition, and crystalline structure and introduction of materials making up the example. The SEM is likewise fit for performing examinations of chose point areas on the example; this methodology is particularly valuable in subjectively or semi-quantitatively deciding synthetic structures. Figure 4 demonstrates the SEM micrographs of the Gd2O3 arranged by combustion synthesis method utilizing urea and glycine as a fuel. The black and white SEM micrograph of the prepared powder indicates that all the particles are looking like agglomerated in homogeneously in different shapes/sizes of the order of nano range.

Figure 4.

Scanning electron microscope image of Gd2O3 phosphor: (A) glycerin fuel and (B) urea fuel.

3.3 TEM result

Transmission electron microscopy (TEM) is an imaging system whereby a light emission is engaged onto an example making a broadened form show up on a fluorescent screen or layer of photographic film or to be distinguished by a CCD camera. The main commonsense transmission electron magnifying instrument was built by Albert Prebus and Lames Hillier at the college of Toronto in 1938 utilizing ideas grew before by Max Knoll and Ernst Ruska. The particle size of the system was determined by high resolution transmission electron microscopy (HRTEM). It is a phase differentiated imaging process because the image formed is due to the scattering of electron waves through a thin surface. In Figure 5, HRTEM micrograph demonstrates a Gd2O3 nanocrystal with a width of 8–10 nm seen all through the particle for both fuels [1, 2, 7].

Figure 5.

Transmission electron microscope image of Gd2O3 phosphor: (A) glycerin fuel and (B) urea fuel.

3.4 Energy dispersive X-ray analysis (EDX)

Elemental investigation of the prepared samples is generally determined by EDX analysis. The spectrum shows the relation between the X-ray energy, which lies in between 10 and 20 eV, and the number of counts per channel by a plot between them in X and Y axes, respectively. An X-ray line is expanded by the reaction of the framework, delivering a Gaussian profile. Energy resolution is characterized as the full width of the crest at half maximum height (FWHM). In the spectrum of both the Gd2O3 samples, intense peak of Gd and O is present, which confirms the formation of Gd2O3 phosphor (Figure 6). For EDX analysis, the entire area of the black and white SEM micrographs was analyzed with EDX mapping and spectrum. The EDX mapping measurements were carried Gd2O3 powders to analyze the composition of the clustered particles [1, 2].

Figure 6.

EDX spectra of Gd2O3 phosphor: (A) glycerin fuel and (B) urea fuel.

3.5 X-ray photoelectron spectroscopy (XPS)

XPS is a surface compositional investigation system that can be utilized to examine the surface chemistry of a material in its as-formed state, or after some treatment, for instance: cracking, cutting, or scratching in air or UHV to uncover the bulk chemistry, ion beam etching to wipe off a few or the majority of the surface defilement or to purposefully uncover further layers of the sample inside and out profiling XPS, presentation to warmth to think about the progressions because of warming, introduction to receptive gases or arrangements, introduction to particle bar embed, and introduction to bright light. The synthetic organization of Gd2O3 nanoparticles was contemplated with X-ray Photoelectron Spectroscopy (XPS), and the test information was broken down utilizing bend fitting. The Gd (3d) level comprised of a turn circle split with the Gd (3d)5/2 top is found at 1186.74 eV (Figure 7). The line shape and pinnacle positions are in great concurrence with prior distributed information on Gd2O3 powder squeezed into the sheet [1].

Figure 7.

The Gd (3d) XPS spectrum of Gd2O3 nanocrystals (reproduced from [1]).

3.6 Raman spectroscopy

To understand the molecular structure, Raman effect has been used, and the obtained Raman data can be compared with the infrared spectra. Raman spectroscopy is very informative to illustrate the structure of the phosphor. It is a nondestructive device to investigate vibrational, rotational, and other low recurrence modes in the frameworks under study. Figure 8 demonstrates the Raman spectra of Gd2O3 obtained by combustion synthesis method. The spectra were recorded at room temperature with an excitation wavelength of 633 nm He-Cd laser. An broad and intense Raman crest at 340 cm−1 along with less extreme peaks was seen at 375, 395, 424, and 451 cm−1. The outcomes are in great concurrence with the recently distributed Raman spectroscopic examinations on Gd2O3 nanoparticles [1].

Figure 8.

Raman spectra of Gd2O3 nanoparticles (reproduced from [1]).

3.7 Photoluminescence spectra and CIE diagrams of Gd2O3 phosphors

The emission spectra of Gd2O3 phosphor prepared with both the fuels have emission peaks at UV and visible region. A slight variation in peaks was observed in emission peaks for both phosphors. The emission spectra of Gd2O3 phosphor prepared by combustion synthesis method have peak at UV region in between 317 and 399 nm along with weak blue band around 450–494 nm, green around 515–586 nm, and red emission centered at 616–625 nm (Figure 9). 6P7/2 → 8S7/2 transition is responsible for the UV emission centered at 317 nm, whereas the visible emissions are due to transition from 6GJ state of Gd3+ [8]. The presence of oxygen vacancy and interstitials also contributes in modified photoluminescence response for oxide-based system [8]. Transition from 6GJ state of Gd3+ ion and 6GJ/6PJ transition is responsible for green and red emissions, respectively (Figure 10).

Figure 9.

Emission spectra of pure Gd2O3 phosphor: (A) urea and (B) glycerin (reproduced from [7]).

Figure 10.

Energy level diagram for emission transitions for pure Gd2O3 phosphor (reproduced from [7]).

To determine the specific color produced by the prepared Gd2O3 phosphor, CIE coordinate diagram was prepared by using MATLAB 7.10.0 (R2010a) software. The CIE coordinates for combustion synthesized Gd2O3 phosphor were found X = 0.207 and Y = 0.206, which resemble with blue color. Effect of annealing on the produced color was determined by the CIE coordinates of Gd2O3 phosphor annealed at 900°C. It was observed that the X and Y coordinates for the annealed sample have same values as freshly prepared samples, and only the change in intensity was observed after annealing (Figure 9) [9].

3.8 Thermoluminescence study of pure Gd2O3 phosphor

The TL response of the Gd2O3 phosphor was recorded under 254 nm UV exposure and 60Co gamma exposure for the phosphors prepared by both urea and glycine fuel. The TL glow curve of phosphors prepared with both the fuels was recorded under 254 nm UV exposure immediately after 5 min exposure time at 6 Cs−1 heating rate. For the combustion synthesized phosphor, the TL glow peak was found at 103°C and 111°C for urea and glycine fuels, respectively. For 1 kGy gamma exposure at 6 Cs−1 heating rate, the TL glow peak was found at 232°C and 221°C (Figure 11) for urea and glycine fueled phosphors, respectively [10].

Figure 11.

TL glow curve for 6 Cs−1 heating rate and 10 min UV exposure with (A) urea fuel and (B) glycerin fuel. TL glow curve for 6°Cs−1 heating rate and 1 kGy gamma exposure (C) urea fuel and (D) glycerin fuel (Reproduced from [8]).

For 275 nmX0.2070.207

Table 1.

X, Y coordinates for CIE diagram for Gd2O3 phosphor.

Chen’s peak shape method was used to determine all the kinetic parameters including order of kinetic, activation energy, shape factor, and so on [4, 5, 6, 11] (Table 1). The activation energy for TL glow curve for combustion synthesized both phosphors has 0.66 eV for UV exposure and 0.71 and 0.72 eV for gamma exposure. Due to gamma exposure, deeper traps were formed, which are responsible for the higher activation energy value. The phosphor follows second-order kinetics as the obtained shape factor value for UV exposure and gamma exposure was in the range of 0.49–0.52 and 0.50–0.54, respectively, which is near to 0.52 for second-order kinetics (Table 2).

ExposureFuelμgE (eV)S (s−1)
UV (254 nm)Urea0.490.661.4 × 1010
Glycerin0.520.661.5 × 1010
Gamma (1kGy)Urea0.540.719.5 × 109
Glycerin0.500.729.7 × 109

Table 2.

Trapping parameters for optimized TL glow curve.

4. Conclusions

The study confirms that the combustion synthesis method is suitable for large-scale production of the phosphor in minimum time. Structural characterization shows that the phosphors have monoclinic structure with particle size in the range of 8–12 nm. Phosphor synthesized by this method has homogenous particle size distribution. X-ray Photoelectron Spectroscopy (XPS) show the Gd (3d) level consists of a spin orbit split doublet, with the Gd (3d)5/2 peak is found at 1186.74 eV. Raman spectra was recorded with excitation of 633 nm wavelength, we found a broad and intense Raman peak at 340 cm−1 along with less intense peaks were observed at 375, 395, 424 and 451 cm−1. The emission spectra have peaks in all UV and visible regions. So that, the phosphor may behave as white light emitting phosphor, which was further confirmed by its CIE coordinates. The CIE coordinates for combustion synthesized Gd2O3 phosphor have values X = 0.207 and Y = 0.206, and for the glycine synthesized Gd2O3 phosphor X = 0.209 and Y = 0.207. The values of CIE coordinates show that the Gd2O3 phosphor prepared by combustion synthesis emits blue color. The TL studies of both the phosphors were carried out under UV and gamma exposure. The activation energy for 0.66 eV and 0.71–0.72 eV for UV exposure and gamma exposure respectively. The value of shape factor μg for all the TL analysis was found in between 0.45 and 0.54, which shows that the phosphors follow the second-order kinetics.


We are very grateful to NIT Raipur for XRD characterization and also thankful to Dr. Mukul Gupta for his co-operation. We are thankful to SAIF, IIT, Bombay and IIT Delhi for other characterization such as SEM, TEM, FTIR, and EDX.

Conflict of interest

The authors declare there is no conflict of interest.

© 2020 The Author(s). Licensee IntechOpen. This chapter is distributed under the terms of the Creative Commons Attribution 3.0 License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

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Raunak Kumar Tamrakar and Kanchan Upadhyay (May 19th 2020). Gd<sub>2</sub>O<sub>3</sub>: A Luminescent Material, Rare Earth Elements and Their Minerals, Michael Aide and Takahito Nakajima, IntechOpen, DOI: 10.5772/intechopen.92310. Available from:

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