Research article

Supercritical hydrothermal synthesis of polycrystalline gadolinium aluminum perovskite materials (GdAlO3, GAP)

  • Received: 15 December 2016 Accepted: 05 March 2017 Published: 06 April 2017
  • The orthorhombic perovskite, Gadolinium aluminum oxide (GdAlO3, GAP) material was successfully prepared by hydrothermal supercritical fluid method using co-precipitated gel of GAP. All experiments were carried out in the pressure and temperature ranges of 100–150 MPa and 180–650 °C respectively. The as-prepared GAP samples were systematically characterized by X-ray diffraction (XRD), scanning electron microscopy (SEM), Fourier transform infrared spectroscopy (FT-IR), X-ray spectroscopy (EDS), thermo gravimetry (TGA) and differential thermo gravimetry analysis (DTA). The XRD profile confirms fully crystalline and orthorhombic nature of as-prepared materials, which is well correlated to the reported results. The SEM studies reveal that the GAP materials synthesized at 650 °C/150 MPa for 92 hrs possesses polycrystalline nature with average particle size in the range of 5–20 µm. The DTA shows a crystallization peak at 361 °C at this temperature the agglomerated GAP gel starts to crystallize into polycrystalline GAP materials. When compared with other methods, like sol-gel and solid-state reactions our crystallization temperature is very much lower and feasible. This work not only demonstrates a simple way to fabricate GAP polycrystalline materials from co-precipitated gels but also shows a possible utilization of same technique for synthesis of other high temperature materials.

    Citation: HN Girish, P Madhusudan, CP Sajan, BV Suresh Kumar, K Byrappa. Supercritical hydrothermal synthesis of polycrystalline gadolinium aluminum perovskite materials (GdAlO3, GAP)[J]. AIMS Materials Science, 2017, 4(3): 540-550. doi: 10.3934/matersci.2017.3.540

    Related Papers:

    [1] Etsana Kiros Ashebir, Berhe Tadese Abay, Taame Abraha Berhe . Sustainable A2BBX6 based lead free perovskite solar cells: The challenges and research roadmap for power conversion efficiency improvement. AIMS Materials Science, 2024, 11(4): 712-759. doi: 10.3934/matersci.2024036
    [2] Asima Adak (Maity), Soumya Mukherjee, Mahua Ghosh Chaudhuri, Siddhartha Mukherjee . Phase evolution, microscopic analysis, optical and dielectric property evaluation of Co-doped BaSnO3 by mechanical mix assisted solid state sintering method. AIMS Materials Science, 2016, 3(3): 1281-1293. doi: 10.3934/matersci.2016.3.1281
    [3] Min Kang, Hai Zhou . Facile Synthesis and Structural Characterization of Co3O4 Nanocubes. AIMS Materials Science, 2015, 2(1): 16-27. doi: 10.3934/matersci.2015.1.16
    [4] Fahmi Astuti, Rima Feisy Azmi, Mohammad Arrafi Azhar, Fani Rahayu Hidayah Rayanisaputri, Muhammad Redo Ramadhan, Malik Anjelh Baqiya, Darminto . Employing Na2CO3 and NaCl as sources of sodium in NaFePO4 cathode: A comparative study on structure and electrochemical properties. AIMS Materials Science, 2024, 11(1): 102-113. doi: 10.3934/matersci.2024006
    [5] Lucangelo Dimesso, Michael Wussler, Thomas Mayer, Eric Mankel, Wolfram Jaegermann . Inorganic alkali lead iodide semiconducting APbI3 (A = Li, Na, K, Cs) and NH4PbI3 films prepared from solution: Structure, morphology, and electronic structure. AIMS Materials Science, 2016, 3(3): 737-755. doi: 10.3934/matersci.2016.3.737
    [6] Leydi J. Cardenas F., Josep Ma. Chimenos, Luis C. Moreno A., Elaine C. Paris, Miryam R. Joya . Enhancing Co3O4 nanoparticles: Investigating the impact of nickel doping and high-temperature annealing on NiCo2O4/CoO heterostructures. AIMS Materials Science, 2023, 10(6): 1090-1104. doi: 10.3934/matersci.2023058
    [7] Xuan Luc Le, Nguyen Dang Phu, Nguyen Xuan Duong . Enhancement of ferroelectricity in perovskite BaTiO3 epitaxial thin films by sulfurization. AIMS Materials Science, 2024, 11(4): 802-814. doi: 10.3934/matersci.2024039
    [8] R.A. Silva, C.O. Soares, R. Afonso, M.D. Carvalho, A.C. Tavares, M.E. Melo Jorge, A. Gomes, M.I. da Silva Pereira, C.M. Rangel . Synthesis and electrocatalytic properties of La0.8Sr0.2FeO3−δ perovskite oxide for oxygen reactions. AIMS Materials Science, 2017, 4(4): 991-1009. doi: 10.3934/matersci.2017.4.991
    [9] M. F. Achoi, S. Kato, N. Kishi, T. Soga . Improved photovoltaic properties of ((CH3NH3)1-xCsx)3Bi2I9: (x = 0-1.0) hybrid perovskite solar cells via a hot immersion method. AIMS Materials Science, 2024, 11(4): 605-619. doi: 10.3934/matersci.2024031
    [10] Silvia Colodrero . Conjugated polymers as functional hole selective layers in efficient metal halide perovskite solar cells. AIMS Materials Science, 2017, 4(4): 956-969. doi: 10.3934/matersci.2017.4.956
  • The orthorhombic perovskite, Gadolinium aluminum oxide (GdAlO3, GAP) material was successfully prepared by hydrothermal supercritical fluid method using co-precipitated gel of GAP. All experiments were carried out in the pressure and temperature ranges of 100–150 MPa and 180–650 °C respectively. The as-prepared GAP samples were systematically characterized by X-ray diffraction (XRD), scanning electron microscopy (SEM), Fourier transform infrared spectroscopy (FT-IR), X-ray spectroscopy (EDS), thermo gravimetry (TGA) and differential thermo gravimetry analysis (DTA). The XRD profile confirms fully crystalline and orthorhombic nature of as-prepared materials, which is well correlated to the reported results. The SEM studies reveal that the GAP materials synthesized at 650 °C/150 MPa for 92 hrs possesses polycrystalline nature with average particle size in the range of 5–20 µm. The DTA shows a crystallization peak at 361 °C at this temperature the agglomerated GAP gel starts to crystallize into polycrystalline GAP materials. When compared with other methods, like sol-gel and solid-state reactions our crystallization temperature is very much lower and feasible. This work not only demonstrates a simple way to fabricate GAP polycrystalline materials from co-precipitated gels but also shows a possible utilization of same technique for synthesis of other high temperature materials.


    1. Introduction

    Ceramic based materials on the Ln2O3-Al2O3 system (Ln-Lanthanide element) have shown their potential applications as a neutron absorber, flux suppressors, and high-temperature container materials [1]. Further, processing of these materials is considerable interest due to their magnetic and optical properties [1,2,3,4]. The study of rare-earth perovskite is of huge interest because of their relatively simple crystal structure with many diverse electric, magnetic, optical, piezoelectric, catalytic, and magnetoresistive properties. Among aluminum perovskite group, several of them are employed has host for solid state-state laser, luminescence system, solid electrolytes, chemical sensors, magnetic refrigeration materials, substrates for high-temperature superconductor deposition, catalyst supports and thermal barrier coatings [5,6]. Gadolinium aluminum perovskite (GAP) are widely used in the preparation of phosphors for color TV tubes [7,8,9,10,11], scintillator [12], regenerator material for sub-4k cryo-coolers [13], Luminescence thermometry with Eu3+ doped GAP [14], as well as a potential host system for materials with oxygen ion conductivity [15,16,17]. Currently, GAP material is under development as a candidate for the neutron absorption and control rod applications. Conventionally, GAP is produced by solid-state reaction of gadolina and alumina powder which involves extensive mechanical mixing followed by heat treatment for prolong duration and sintering at relatively high temperatures (1650–1700 ℃) [18,19]. To avoid the problem associated with solid-state synthesis of GAP powder, several wet-chemical techniques, such as polymerized complex route, combustion system, sol-gel, flux methods, melt technique, citrate-nitrate solution and microwave technique have been used to synthesize GAP [7,9,15,20,21,22,23,24,25,26,27]. However, these are high-temperature methods which consume a lot of energy and lead to certain thermally induced strain in the resultant products thereby affecting their quality and indorsing crystal defects. In our previous investigation, we reported the synthesis of the pure phase of aluminum perovskite materials using supercritical hydrothermal technique [28,29,30]. The supercritical hydrothermal technique (SHT) has advantages over mild hydrothermal technique (MHT) to obtain GdAlO3 powder with high purity and homogeneity, fine crystallinity, narrow size distribution and controlled particle morphology. Beyond the supercritical point (373.946 ℃/22.064 MPa) in the liquid–vapor space, water exists as small but liquid-like (associated) hydrogen-bonded clusters dispersed within a gas-like (dissociated) phase [31]. Previously, we had investigated hydrothermal synthesis of GAP particles with significance to their phase formation [32]. In this paper, we extend our previous research work and have varied the experimental environments and discussed about the favorable condition employed for synthesis of orthorhombic GAP phase. Our preparation conditions are much milder and simpler than those of conventional solid-state method, which require high-temperature heat treatment. Further, the TG-DSC behavior of co-precipitated gel during the formation of GAP polycrystalline phase has been discussed. The SEM images of as-prepared GAP materials are compared and discussed with co-precipitated GAP gel starting materials. The particle size and morphology of the GAP materials synthesized at 650 ℃/150 MPa are quite different from our previously reported results. The as-prepared samples were subjected to systematic characterization using thermal analysis/differential scanning calorimetry (TG/DSC), powder X-ray diffraction (XRD), Fourier transform infrared spectroscopy (FTIR), scanning electron microscope and energy dispersive X-ray spectroscopy (SEM/EDAX).


    2. Materials and Method


    2.1. Materials

    Gadolinium oxide (LOBA Chemie Co. Ltd, purity 99.9%, extra pure), aluminum oxide (LOBA Chemie Co. Ltd., purity 99%, neutral), nitric acid (LOBA Chemie Co. Ltd., purity 69%, pure), ammonium solution (LOBA Chemie Co. Ltd.). All the reagents were of analytical grade and used without further purification. Deionized water was used for post treatment processes.


    2.2. Hydrothermal Synthesis of Gadolinium Aluminum Perovskite (GdAlO3, GAP)

    Synthesis of gadolinium aluminate (GdAlO3, GAP) polycrystalline ceramics materials by hydrothermal supercritical technique were carried out using externally heated (Tuttle-Roy test tube type) pressure vessels. The co-precipitated gels of gadolinium and aluminum were used as precursors. These co-precipitate gels are more sensitive and highly reactive materials for the synthesis of perovskite materials. The possible reaction mechanism for the formation of GAP co-precipitate gel is as shown:

    Gd2O3+6HNO32Gd(NO3)3+3H2O (1)
    Al2O3+6HNO32Al(NO3)3+H2O (2)
    Gd(NO3)3+Al(NO3)3+6HN4OHGd(OH)3+Al(OH)3+6HN4NO3 (3)
    Gd(OH)3+Al(OH)31/2Gd2O3+1/2Al2O3+3H2O (4)
    1/2Gd2O3+1/2Al2O3GdAlO3 (5)

    The schematic flow chart for the preparation of co-precipitation gel using respective raw materials is illustrated in Figure 1. Similar, method was also adopted by Basavalingu et al. for the synthesis of orthorhombic YAlO3 [28] and, Hamilton & Henderson for preparation of silicate minerals [33]. The experimental details of hydrothermal runs on the synthesis of GAP materials are shown in Table 1. The experiments were carried out using the conventional test tube type Tuttle-Roy externally heated pressure vessels in the pressure and temperature range of 100–150 MPa and 180–650 ℃, respectively. The starting co-precipitated gels were homogeneously mixed and were taken in a sealed gold tube of 50–60 mm in length and 4.5 mm in outer diameter and with wall thickness of 0.1 mm. The capsules were carefully sealed with arc welding after taking the appropriate quantity of starting charge comprising of both solids and liquids. The capsules were checked for leakage before placing into the vessel by keeping them for extended heating in a hot air oven at 100 ℃ for check any weight difference. The capsules showing any weight loss during this process were discarded. The duration of the experimental runs was 48 to 92 hours, and later the vessels were quenched by compressed air blast. After the desired experimental condition the run products was carefully removed by cutting the capsules, was recovered, washed with distilled water, ultrasonicated and dried in hot air oven at 70 ℃ for 8 hours. The resultant product obtained was subjected to further characterization using different analytical techniques.


    2.3. Material Characterization

    The reaction process was studied by using differential scanning calorimetry and thermogravimetric analyses (DSC-TG, Netzsch STA 449F3, Germany) for prepared co-precipitated gel from RT (room temperature) to 1400 ℃. The XRD analysis was carried out to study the crystalline phase at ambient temperature using Rigaku-D/MAX-2400 diffractometer with CuKα radiation from 2θ = 0° to 70° at a step of 0.05°. The infrared spectra in the range of 4000–400 cm−1 were recorded using FT-IR spectrophotometer, Jasco 460 plus, Japan. Energy dispersive X-ray analyses (EDAX) were used for quantitative analysis and scanning electron microscope (SEM) model JEOL JSM-6380LA was used for studying the morphology and microstructure of the as-prepared samples.

    Figure 1. Schematic diagram have different steps for preparation of GAP co-precipitated gel.

    3. Results and Discussion


    3.1. TG-DSC Curve Analysis of Co-precipitate Gel

    The thermogravimetric and differential thermal analysis of co-precipitated gel were carried out using a Netzsch STA 449F3, Germany in the temperature range 20–1400 ℃ at a heating rate of 10 ℃/min under Argon atmosphere and the results are illustrated in Figure 2. The TG-DSC profile clearly depicts that during the preparation of co-precipitate gel which involves different step like aging, drying, and heating at 600 ℃, H2O and volatile compound like NH3 were released. It was also observed that there was a small endothermic reaction at 75.6 ℃ which is attributed to the release of a trace amount of moisture and NH3 gas. Further, major weight loss was observed at the temperature range between 300–400 ℃. This is due to the evolution of gasses such as NO, NH3, and NO2. The DTA shows a crystallization peak at 361 ℃ at this temperature the agglomerated GAP gel starts to crystallize into polycrystalline GAP materials. At the region of 1148 ℃, a small exothermic peak was observed which is associated with significant weight change in the sample complete formation of orthorhombic GAP. The crystallization temperature is lower when compared to other methods, like solid-state reactions [19].

    Figure 2. TG and DSC profile curves of precursor sample recorded from ambient to 1400 ℃ with a heating rate of 10 ℃/min under Argon atmosphere.
    Table 1. Experimental detail for the synthesis of GAP in different experimental condition (CPG = Co-precipitated gel).
    Exp. No. Precursors Temp. (℃) Pressure (MPa) Duration (hrs.) Run Product
    HN-6 Gd2O3 + Al2O3 + H2O 180 autonomous 72 Gd2O3 + Al2O3 powder
    HN-10 Gd2O3 + Al2O3 + H2O 200 autonomous 48 Gd2O3 + Al2O3 powder
    HN-12 Gd2O3 + Al2O3 + H2O 200 autonomous 72 Gd2O3 + Al2O3 powder
    HN-16 CPG + H2O 200 autonomous 72 Al2O3 powder
    HN-21 CPG + H2O 400 autonomous 72 Al2O3 powder
    HN-25 CPG + H2O 400 100 48 Gd2O3 + Al2O3 mix phase
    HN-31 CPG + H2O 500 100 48 Gd2O3 + Al2O3 mix phase
    HN-37 CPG + H2O 500 100 72 Gd2O3 + Al2O3 mix phase
    HN-39 CPG + H2O 600 120 72 GAP + Al2O3 phase
    HN-41 CPG + H2O 600 120 92 GAP + Al2O3 phase
    HN-47 CPG + H2O 650 150 92 GAP phase
    HN-49 CPG + H2O 650 150 92 GAP phase
     | Show Table
    DownLoad: CSV

    3.2. X-ray Diffraction

    The XRD patterns of the co-precipitated gel, synthesized GAP and reported GAP standard material are shown in Figure 3. The XRD pattern of co-precipitated gel used as the starting material for GAP synthesis was amorphous in nature without any diffraction peaks. On the other hand, the XRD pattern of as-prepared GAP polycrystalline materials matches well with already reported PDF, 46-0395 of orthorhombic GdAlO3 phase [34]. The peaks in the region 23.87, 33.98, 42.08, 48.77, 55.09 and 60.98 corresponds to (002), (112), (202), (220), (114) and (312) planes, respectively. The resultant X-ray pattern is similar to the X-ray diffraction data of GAP synthesized by solution combustion method [10,24], sol-gel method where the samples were repeatedly dried and sintered at 1000 ℃ for 10 hrs [35], nanocrystalline GdAlO3 synthesized in citrate gel method in absence of oxygen at 1200 ℃ [23], reverse micelle method where calculations was carried at temperature above 1000 ℃ [36], synthesized Eu3+ doped GdAlO3 in solid state reaction above 1000 ℃ [19] and Tb3+ and Bi3+ doped GdAlO3 synthesized by solvothermal reaction method at 1000 ℃ [8]. It was observed that at a temperature less than 600 ℃, and 150 MPa pressure, the resultant products were a mixed phase and the small peak arise at 23.8 theta region matches with Al2O3 impurity phase (not shown). The refinement of lattice parameters was done using CHEKCELL software and obtained lattice parameters was compared with the reported data which is shown in Table 2. From the XRD pattern of the GAP, it is clear that the synthesized compound possess highly crystallized pure phase. The cell parameter of the synthesized GAP is different in a small amount which might be due to the experimental conditions.

    Figure 3. X-ray diffraction pattern: a) reported a pattern of GAP, JCPDS = 46-0395 [34], b) Co-precipitated gel of GAP and c) Synthesized GAP at 650 ℃/150 MPa at 92 hrs.
    Table 2. Refined lattice parameters of synthesized GAP compared with reported data.
    Compound a-axis (Å) b-axis (Å) c-axis (Å) Cell volume (Å3)
    GAP (PDF = 46-0395) [34] 5.251 5.301 7.445 207.27
    Synthesized GAP 5.243 5.302 7.441 207.12
     | Show Table
    DownLoad: CSV

    3.3. Infrared Spectra and SEM with EDAX Analysis

    To investigate the chemical composition and chemical bonding of co-precipitate gel of GAP and polycrystalline GAP materials, FT-IR was carried out and the corresponding spectra are shown in Figure 4. In the FT-IR spectrum of the co-precipitate gel (Figure 4a), there is a broad strong absorption at around 3450 cm−1 and a narrow band at 1635 cm−1 which are assigned to the stretching and bending modes of absorbed water, respectively. Figure 4b presents FT-IR spectra of the GAP sample synthesized at 650 ℃/150 MPa condition. The small absorption band from 3000 cm−1 to 3800 cm−1 corresponds to the OH mode which might be due to the water molecules absorbed at room temperature. On the other hand, –C=C– bond in the synthesized GAP material is represented by the band at 1570 cm−1 which might be due to the adsorption of atmospheric carbon (Figure 4b). The band appearing at 1381 cm−1 corresponds to vibration modes of NO3 groups. The band observed in the low-frequency region of the spectrum, corresponds to the lattice vibration mode which is attributed to typical gadolinium oxygen (Gd–O) vibration at 520 cm−1. The band frequencies at 660 and 465 cm−1 which are typical of the Al–O stretching characteristic vibrations in the perovskite structure compounds [37,38,39,40].

    Figure 4. FT-IR spectrum: a) Co-precipitate gel of GAP at room temperature, b) Synthesized GAP at 650 ℃/150 MPa at 92 hrs.

    The morphology and the particle size of the resultant product were analyzed by SEM. The SEM images of the prepared co-precipitate gel were agglomerate in nature (Figure 5a and 5b) which is in agreement with the XRD result which showed amorphous nature. The SEM image of GAP materials synthesized at 650 ℃/150 MPa for 92 hrs possesses polycrystalline nature with the orthorhombic crystal structure (Figure 5c and 5d). The SEM images further reveal that the average particle size of synthesized GAP crystals is in a range of 5–20 µm, which clearly shows that are as-prepared products are homogeneous material with polycrystalline nature. Furthermore, it is worth to reveal that the morphology of our synthesized GAP material is quite difference than GdAlO3 synthesized from sol-gel technique [22] and our previous results [32]. Based on XRD and SEM studies it was conformed that the phase formation under hydrothermal supercritical condition mainly depends on the nature of precursor materials, crystallization temperature and pressure. The atomic percentage of elements present in the as-prepared sample was performed at magnification 200× high voltage of 15.0 kV. The atomic percentage of elements, i.e, Gd, Al and O present in the sample is shown in Table 3. From the EDAX analysis, it is clear that the synthesized sample is free from impurities and doesn't contain any foreign materials. Furthermore, the morphological study in support with compositional study confirms that these crystals possess nominal phase stoichiometry and the supercritical fluids generated inside the gold capsules has greatly influenced in the resultant morphology of the crystals and also maintain their chemical composition.

    Figure 5. SEM images: a & b) as prepared Co-precipitate gel of GAP; c & d) synthesized GAP at 650 ℃/150 MPa for 92 hrs.
    Table 3. Percentage composition of GAP.
    Run product O (at.%) Al (at.%) Gd (at.%) Total (at.%)
    GAP 20.72 25.56 53.72 100
     | Show Table
    DownLoad: CSV

    4. Conclusions

    In summary, we have reported the synthesis of polycrystalline GAP materials under the influence on supercritical hydrothermal fluid condition. The composition of the starting charge materials and experimental condition play an important role in preparation of GAP crystals. So far it was difficult to synthesize single phase GAP materials due to their difficulty in controlling stoichiometric composition. In this paper, we have conducted the experiments at pressure and temperature ranges of 100–150 MPa and 180–650 ℃ respectively. Further, the as-prepared GAP samples were systematically characterized by different analytical techniques. The XRD results of samples prepared at 650 ℃/150 MPa shows well crystalline orthorhombic phase and SEM shows the samples are of 5–20 µm in size. The synthesis temperature of our experiments was lower than other methods, like sol-gel and solid-state reactions. The current strategy not only demonstrates a simple possible way to fabricate the orthorhombic phase of GAP polycrystalline material from co-precipitated gel, but also shows a prospect for further investigations on the synthesis of similar rare-earth doped oxides for customized applications.


    Conflict of Interest

    The authors declare that there is no conflict of interest.


    [1] Attfield JP (2001) Structure–property relations in doped perovskite oxides. Int J Inorg Mater 3: 1147–1152. doi: 10.1016/S1466-6049(01)00110-6
    [2] Atwood DA, Yearwood BC (2000) The future of aluminium chemistry. J Organomet Chem 600: 186–197. doi: 10.1016/S0022-328X(00)00147-9
    [3] Cashion JD, Cooke AH, Hawkes JFB, et al. (1968) Magnetic Properties of Antiferromagnetic GdAIO3. J Appl Phys 39: 1360–1361. doi: 10.1063/1.1656304
    [4] Cashion JD, Cooke AH, Leask MJM, et al. (1968) Crystal Growth and Magnetic Susceptibility of Some Rare-Earth Compounds. Part 2. Magnetic Susceptibility Measurements on a Number of Rare-Earth Compound. J Mater Sci 3: 402–407.
    [5] Vonka P (2009) A method for the estimation of the enthalpy of formation of mixed oxides in Al2O3-Ln2O3 systems. J Solid State Chem 182: 744–748. doi: 10.1016/j.jssc.2008.12.016
    [6] Hayashi H, Inaba H, Matsuyama M, et al. (1999) Structural consideration on the ionic conductivity of perovskite-type oxides. Solid State Ionics 122: 1–15. doi: 10.1016/S0167-2738(99)00066-1
    [7] Han SD, Khatkar SP, Taxak VB, et al. (2006) Combustion synthesis and luminescent properties of Eu3+-doped LnAlO3 (Ln = Y and Gd) phosphors. Mater Sci Eng B 127: 272–275. doi: 10.1016/j.mseb.2005.10.016
    [8] Park JY, Jung HC, Raju GSR, et al. (2010) Enhanced green emission from Tb3+–Bi3+ co-doped GdAlO3 nanophosphors. Mater Res Bull 45: 572–575. doi: 10.1016/j.materresbull.2010.01.016
    [9] Oliveira HHS, Cebim MA, Da Silva AA, et al. (2009) Structural and optical properties of GdAlO3:RE3+ (RE = Eu or Tb) prepared by the Pechini method for application as X-ray phosphors. J Alloy Compd 488: 619–623. doi: 10.1016/j.jallcom.2009.04.099
    [10] Jisha PK, Naik R, Prashantha SC, et al. (2015) Facile combustion synthesized orthorhombic GdAlO3:Eu3+ nanophosphors: Structural and photoluminescence properties for WLEDs. J Lumin 163: 47–54. doi: 10.1016/j.jlumin.2015.03.006
    [11] Selvalakshmi T, Venkatesan P, Wu SP, et al. (2017) Gd2O3:RE3+ and GdAlO3:RE3+ (RE = Eu, Dy) Phosphor: Synthesis, Characterization and Bioimaging Application. J Nanosci Nanotechno 17: 1178–1184. doi: 10.1166/jnn.2017.12578
    [12] Verweij JWM, Cohen-Adad MT, Bouttet D, et al. (1995) Luminescence properties of GdAIO3:Ce powders. Dependence on reduction conditions. Chem Phys Lett 239: 51–55.
    [13] Qiu LM, Numazawa T, Thummes G (2001) Performance improvement of a pulse tube cooler below 4 K by use of GdAlO3 regenerator material. Cryogenics 41: 693–696. doi: 10.1016/S0011-2275(01)00146-1
    [14] Lojpur V, Ćulubrk S, Medić M, et al. (2016) Luminescence thermometry with Eu3+ doped GdAlO3. J Lumin 170: 467–471. doi: 10.1016/j.jlumin.2015.06.032
    [15] Sinha A, Sharma BP, Gopalan P (2006) Development of novel perovskite based oxide ion conductor. Electrochim Acta 51: 1184–1193. doi: 10.1016/j.electacta.2005.06.009
    [16] Sinha A, Näfe H, Sharma BP, et al. (2008) Study on Ionic and Electronic Transport Properties of Calcium-Doped GdAlO3. J Electrochem Soc 155: B309–B314. doi: 10.1149/1.2829877
    [17] Luo H, Bos AJJ, Dorenbos P (2016) Controlled Electron–Hole Trapping and Detrapping Process in GdAlO3 by Valence Band Engineering. J Phys Chem C 120: 5916–5925.
    [18] Cao G (2004) Nanostructures and Nanomaterials: Synthesis, Properties and Applications, London: Imperial College Press.
    [19] Upadhyay K, Tamrakar RK, Dubey V (2015) High temperature solid state synthesis and photoluminescence behavior of Eu3+ doped GdAlO3 nanophosphor. Superlattice Microst 78: 116–124. doi: 10.1016/j.spmi.2014.11.030
    [20] Raju GSR, Park JY, Jung HC, et al. (2009) Synthesis and luminescent properties of low concentration Dy3+:GAP nanophosphors. Opt Mater 31: 1210–1214. doi: 10.1016/j.optmat.2008.12.015
    [21] Gao H, Wang Y (2007) Preparation of (Gd, Y)AlO3:Eu3+ by citric-gel method and their photoluminescence under VUV excitation. J Lumin 122–123: 997–999.
    [22] Cizauskaite S, Reichlova V, Nertavicience G, et al. (2007) Sol-gel preparation and characterization of perovskite gadolinium aluminates. Mater Sci-Poland 25: 755–765.
    [23] Sinha A, Sharma BP, Näfe H, et al. (2010) Synthesis of gadolinium aluminate powder through citrate gel route. J Alloy Compd 502: 396–400. doi: 10.1016/j.jallcom.2010.04.179
    [24] Sinha A, Nair SR, Sinha PK (2011) Single step synthesis of GdAlO3 powder. J Alloy Compd 509: 4774–4780. doi: 10.1016/j.jallcom.2011.01.156
    [25] Catunda T, Andreeta JP, Castro JC (1986) Differential interferometric technique for the measurement of the nonlinear index of refraction of ruby and GdAlO3:Cr+3. Appl Optics 25: 2391–2395. doi: 10.1364/AO.25.002391
    [26] Harada Y, Uekawa N, Kojima T, et al. (2009) Fabrication of dense material having homogeneous GdAlO3-Al2O3 eutectic-like microstructure with off-eutectic composition by consolidation of the amorphous. J Eur Ceram Soc 29: 2419–2422. doi: 10.1016/j.jeurceramsoc.2009.01.017
    [27] Selvam MP, Rao KJ (2000) Microwave synthesis and consolidation of gadolinium aluminum perovskite, a ceramic extraordinaire. Adv Mater 12: 1621–1624. doi: 10.1002/1521-4095(200011)12:21<1621::AID-ADMA1621>3.0.CO;2-X
    [28] Basavalingu B, Girish HN, Byrappa K, et al. (2008) Hydrothermal synthesis and characterization of orthorhombic yttrium aluminum perovskites (YAP). Mater Chem Phys 112: 723–725. doi: 10.1016/j.matchemphys.2008.06.049
    [29] Girish HN, Vijayakumar MS, Devaraju MK, et al. (2009) Hydrothermal Synthesis and Characterization of Neodymium doped Yttrium Aluminum Perovskite (Nd:YAP). Indian Mineral 43: 162–168.
    [30] Basavalingu B, Kumar MSV, Girish HN, et al. (2013) Hydrothermal synthesis and characterization of rare earth doped yttrium aluminium perovskite-R:YAlO3 (R = Nd, Eu & Er). J Alloy Compd 552: 382–386. doi: 10.1016/j.jallcom.2012.10.091
    [31] Rukes B, Dooley RB (2001) Guideline on the Use of Fundamental Physical Constants and Basic Constants of Water. International Association for the Properties of Water and Steam, Gaithersburg, Maryland, USA, 1–7.
    [32] Girish HN, Basavalingu B, Shao GQ, et al. (2015) Hydrothermal synthesis and characterization of polycrystalline gadolinium aluminum perovskite (GdAlO3, GAP). Mater Sci-Poland 33: 301–305
    [33] Hamilton DL, Henderson CMB (1968) The preparation of silicate compositions by a gelling method. Mineral Mag 36: 832–838. doi: 10.1180/minmag.1968.036.282.11
    [34] Wang P (1994) Shanghai Inst. of Ceramics, Chinese Academy of Science, Shanghai, China.
    [35] Cizauskaitė S, Špakauskaitė G, Beganskienė A, et al. (2006) A comparative study of GdAlO3 perovskite prepared by the sol-gel method using different complexing agents. Chemija 17: 40–45.
    [36] Chandradass J, Kim KH (2010) Reverse Micelle-Directed Synthesis of GdAlO3 Nanopowders. Mater Manuf Process 25: 1428–1431. doi: 10.1080/10426914.2010.499744
    [37] Schrader B (1995) Infrared and Raman Spectroscopy, Method and Application.
    [38] Nakamoto K (1986) Infrared and Raman Spectroscopy of Inorganic and Coordination Compounds.
    [39] Vaqueiro P, López-quintela MA (1998) Synthesis of yttrium aluminium garnet by the citrate gel process. J Mater Chem 8: 161–163. doi: 10.1039/a705635d
    [40] Chroma M, Pinkas J, Pakutinskiene I, et al. (2005) Processing and characterization of sol-gel fabricated mixed metal aluminates. Ceram Int 31: 1123–1130. doi: 10.1016/j.ceramint.2004.11.012
  • This article has been cited by:

    1. Shiyu Dai, Gang Wang, Pengyuan Qi, Xiaochen Xu, Lili Jiang, Jingyu Zhong, Shuo Yuan, Lei Wang, Study of gadolinium aluminate nanoparticles with perovskite structure prepared by citric acid chelation method, 2020, 7, 2053-1591, 125008, 10.1088/2053-1591/abcdd7
    2. Ellen Hertle, Liudmyla Chepyga, Andres Osvet, Christoph J Brabec, Miroslaw Batentschuk, Stefan Will, Lars Zigan, (Gd,Lu)AlO3:Dy3+ and (Gd,Lu)3Al5O12:Dy3+ as high-temperature thermographic phosphors, 2019, 30, 0957-0233, 034001, 10.1088/1361-6501/aafcac
    3. Pengyuan Qi, Jingyu Zhong, Shiyu Dai, Weimin Ma, Lili Jiang, Hydrothermal-solid state synthesis of Gadolinium aluminate nano whiskers with alkaline mineralizer, 2020, 7, 2053-1591, 035021, 10.1088/2053-1591/ab7dfd
    4. M. Rakesh, B. R. Narendra Babu, A. P. Gnana Prakash, N. S. Prema, Ashwin C. Gowda, B. S. Madhukar, M. G. Vijay Kashimatt, T. M. Pradeep, B. V. Suresh Kumar, Puttaswamy Madhusudan, Fabrication of lead zirconate titanate-based polyvinylidene fluoride polymer nano-composites: microcrystalline, morphological and electrical studies, 2023, 34, 0957-4522, 10.1007/s10854-022-09768-4
    5. Corneliu Doroftei, Liviu Leontie, Porous Nanostructured Gadolinium Aluminate for High-Sensitivity Humidity Sensors, 2021, 14, 1996-1944, 7102, 10.3390/ma14227102
    6. Martin Fabián, Blanca I. Arias-Serrano, Jaroslav Briančin, Aleksey Yaremchenko, Mechanosynthesis and electrical conductivity of undoped and calcium-substituted GdAlO3 perovskites, 2023, 965, 09258388, 171374, 10.1016/j.jallcom.2023.171374
    7. Daniel Nolasco‐Altamirano, Alejandro Alonso‐Sotolongo, José Francisco Benavente‐Cuevas, Ricardo García‐Salcedo, Olivia Amanda García‐Gardunño, J. Zarate‐Medina, Virgilio Correcher, Teodoro Rivera‐Montalvo, Kinetic Parameters Analysis of GdAlO3 Based on Thermoluminescent Phenomenon, 2024, 0370-1972, 10.1002/pssb.202400381
    8. Hafsa Mansha, Kashf Zaman, Touseef Ahmad, Muhammad Khalid, M. Ahsan Masood, M. Shahid Sharif, M.A.K. Yousaf Shah, Nabeela Akbar, Yuzheng Lu, Jun Wang, Bin Zhu, Amorphous oxide Gd-alumina electrolyte for low-temperature ceramic fuel cells, 2025, 101, 03603199, 1, 10.1016/j.ijhydene.2024.12.350
  • Reader Comments
  • © 2017 the Author(s), licensee AIMS Press. This is an open access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/4.0)
通讯作者: 陈斌, bchen63@163.com
  • 1. 

    沈阳化工大学材料科学与工程学院 沈阳 110142

  1. 本站搜索
  2. 百度学术搜索
  3. 万方数据库搜索
  4. CNKI搜索

Metrics

Article views(6200) PDF downloads(1073) Cited by(8)

Article outline

Figures and Tables

Figures(5)  /  Tables(3)

/

DownLoad:  Full-Size Img  PowerPoint
Return
Return

Catalog