Synthesis of nano-sized particles of thulium-doped gadolinium sesquioxide is reported. The nanopowder was obtained by laser ablation of solid target composed of a mixture of Tm2O3 and Gd2O3 powders using radiation of pulse-periodical CO2 laser. Morphological features, structural characteristics of nanoparticles and their densification behavior were investigated. It was shown that the as-synthesized nanopowder consists of loosely agglomerated particles with spherical shape and a diameter from 10 to 40 nm. It was revealed that the obtained sample is in the form of solid solution of Tm2O3 in Gd2O3 with monoclinic crystalline phase exhibiting the following lattice parameters: a = 14.095 Å; b = 3.571 Å c = 8.758 Å β = 100.182 °. Using X-ray diffraction analysis it was determined that, as opposed to other rare-earth sesquioxides (for instance, Y2O3 and Lu2O3), the phase transformation of monoclinic modification into cubic modification was not observed under thermal treatment at a temperature up to 1200 °C. This was also confirmed by an absence of stepwise variation in density of Tm:Gd2O3 compact which was evident for Gd2O3 sample prepared from powder with cubic phase and micro-sized particles. © Published under licence by IOP Publishing Ltd.The reported study was funded by RFBR and Sverdlovsk region, project number 20-48-660039

Maksimov, R. N.

Osipov, V. V.

Shitov, V. A.

Tikhonov, E. V.

Vasin, D. A.

Journal of Physics Conference Series

Institutional repository of Ural Federal University named after the first President of Russia B.N.Yeltsin

Journal of Physics: Conference SeriesPAPER • OPEN ACCESSLaser ablation synthesis and characteristics of Tm-doped Gd2O3 nanoparticlesTo cite this article: V V Osipov et al 2021 J. Phys.: Conf. Ser. 1942 012026 View the article online for updates and enhancements.You may also likeFirst-principles study of crystal structure,elastic stiffness constants, piezoelectricconstants, and spontaneous polarizationof orthorhombic Pna21-M2O3 (M = Al, Ga,In, Sc, Y)Kazuhiro Shimada-Atomic interface structure of bixbyite rare-earth sesquioxides grown epitaxially onSi(1 1 1)Michael Niehle and Achim Trampert-Band structures of RE2O3:Eu (RE = Lu, Y,Sc) from perspective of spin-polarizedquasi-particle approximationShiJie Chen, Yaoping Xie, He Feng et al.-This content was downloaded from IP address 212.193.94.28 on 14/04/2022 at 06:28Content from this work may be used under the terms of the Creative Commons Attribution 3.0 licence. Any further distributionof this work must maintain attribution to the author(s) and the title of the work, journal citation and DOI.Published under licence by IOP Publishing LtdNMAT 2020Journal of Physics: Conference Series 1942 (2021) 012026IOP Publishingdoi:10.1088/1742-6596/1942/1/0120261      Laser ablation synthesis and characteristics of Tm-doped Gd2O3 nanoparticles V V Osipov1, D A Vasin1, E V Tikhonov1, R N Maksimov1,2, and V A Shitov1 1Institute of Electrophysics UrB RAS, 106 Amundsen St., Ekaterinburg, Russia; 2Ural Federal University named after the first President of Russia B.N. Yeltsin, 19 Mira St., Ekaterinburg, Russia. Corresponding author’s e-mail: osipov@iep.uran.ru Abstract. Synthesis of nano-sized particles of thulium-doped gadolinium sesquioxide is reported. The nanopowder was obtained by laser ablation of solid target composed of a mixture of Tm2O3 and Gd2O3 powders using radiation of pulse-periodical CO2 laser. Morphological features, structural characteristics of nanoparticles and their densification behavior were investigated. It was shown that the as-synthesized nanopowder consists of loosely agglomerated particles with spherical shape and a diameter from 10 to 40 nm. It was revealed that the obtained sample is in the form of solid solution of Tm2O3 in Gd2O3 with monoclinic crystalline phase exhibiting the following lattice parameters: a=14.095 Å; b=3.571 Å c=8.758 Å; β=100.182 °. Using X-ray diffraction analysis it was determined that, as opposed to other rare-earth sesquioxides (for instance, Y2O3 and Lu2O3), the phase transformation of monoclinic modification into cubic modification was not observed under thermal treatment at a temperature up to 1200 °C. This was also confirmed by an absence of stepwise variation in density of Tm:Gd2O3 compact which was evident for Gd2O3 sample prepared from powder with cubic phase and micro-sized particles. 1. Introduction In recent years optical materials based on rare-earth sesquioxides doped with Yb3+, Tm3+ or Er3+ have attracted considerable interest owing to potential utilization as gain media of high-power solid-state lasers [1]. Compared to Y2O3, Lu2O3 and Sc2O3 gadolinium sesquioxide (Gd2O3) of cubic modification possess relatively low phonon energy (νmax=569 cm-1) [2] which can reduce undesirable multiphonon relaxation rates. However, polymorphic phase transition from the cubic phase into the monoclinic phase at the temperatures of about 1300 °C induces inability of melt growth and sintering of transparent ceramics using traditional methods. Therefore insufficient attention has been paid to the fabrication and investigation of optical materials based on cubic Gd2O3.  In turn, the utilization of ultrafine powders exhibiting high surface free energy (sinterability) and modern consolidation technologies enabled access to the synthesis of high-melting point polycrystalline materials such as MgAl2O4, Y2O3 and Y3Al5O12 with good optical quality and submicron-grained structure at the temperatures not higher than 1300 °C [3–7]. In this work we report on the synthesis of nano-sized particles based on Gd2O3 by laser ablation of solid target in air flow and investigation of their morphology, crystalline structure and densification behavior.  NMAT 2020Journal of Physics: Conference Series 1942 (2021) 012026IOP Publishingdoi:10.1088/1742-6596/1942/1/0120262      2. Materials and methods Nano-sized particles of Tm-doped Gd2O3 were synthesized in the Institute of Electrophysics UrB RAS by laser ablation of the corresponding solid target by radiation of pulse-periodical CO2 laser “LAERT”. The details of experimental setup were described elsewhere [8]. In order to prepare laser target for ablation, Tm2O3 and Gd2O3 powders (99.99 mass%, Lanhit Company, Russia) composed of micro-sized particles were dry mixed together for 24 h to form Tm0.1Gd1.9O3 mixture. The obtained blend was then compacted into cylindrical-shaped target with a diameter of ~66 mm by uniaxial static pressing at 10 MPa and pre-sintered at 1100 °C for 5.5 h in air. Typical laser parameters during the synthesis of nanopowder were as follows: pulse energy – 0.9 J, pulse duration – 330 μs, pulse repetition rate – 500 Hz, peak power –7 kW, average power – 450 W. The laser beam was focused into 0.75 mm × 0.9 mm-sized elliptical spot by a KCl lens with a power density of 1.3 MW/cm2. The linear velocity of laser beam movement was 35 cm/s. The production rate of nanopowder was 19 g/h.  The morphological features of the as-synthesized nanoparticles was observed using a JEOL JEM 2100 (JEOL Ltd., Japan) transmission electron microscope (TEM). The chemical composition of the nanopowder was analyzed using an Optima 2100 DV inductively coupled plasma mass spectrometer (ICP MS, Perkin Elmer, USA). The phase composition of nanopowder samples was examined by an X-ray diffractometer Bruker D8 Discover (Bruker AXS, Germany) using Cu Kα radiation. In order to investigate densification behavior, around 700 mg of the as-obtained nanopowder were uniaxially pressed at 50 MPa to form 8-mm-diameter and about 4-mm-height pellet with density of about 3.22 g/cm3. The compact was heated up to 1550 °C with a heating rate of 3 °C/min using a horizontal using a dilatometer NETZSCH DIL 402C (NETZSCH, Germany). Another powder compact with a density of 4.08 g/cm3 was prepared from micro-sized Gd2O3 particles by uniaxial pressing at 200 MPa for comparison. 3. Results and discussion Inductively coupled plasma mass spectrometry (ICP MS) was carried out to determine the chemical compositions of the as-synthesized Tm:Gd2O3 nanoparticles and possible deviation with respect to the composition of laser target. According to ICP MS analysis, the compositions of nanopowder and the corresponding laser target were Tm0.08Gd1.92O3 and Tm0.102Gd1.898O3, respectively. A slight deviation from the desired ratio is probably due to the difference in the evaporation rates of Tm2O3 and Gd2O3.  Figure 1 shows transmission electron microscopy image of Tm:Gd2O3 nanopowder. One can see that the particles are weakly agglomerated, have mostly single-crystalline structure and spherical shape while their size is in the range from 10 to 40 nm. NMAT 2020Journal of Physics: Conference Series 1942 (2021) 012026IOP Publishingdoi:10.1088/1742-6596/1942/1/0120263       Figure 1. TEM image showing morphology of Tm:Gd2O3 nanopowder synthesized by laser ablation.  Figure 2 shows X‐ray diffractograms of the as-synthesized and calcined Tm:Gd2O3 nanoparticles in the 2θ range between 20° and 65°. The observed diffraction patterns can be well indexed to the monoclinic phase of Gd2O3 (PDF No. 00-042-1465), space group C2/m irrespective of the calcination temperature (Table 1). The substitution of Gd3+ cations for Tm3+ cations in the Gd2O3 matrix leads to a certain lattice disorder and compression of crystalline structure because the effective ionic radius of Tm3+ (0.88 Å) is smaller than that of Gd3+ (0.94 Å). Consequently, the diffraction peaks of the Tm0.08Gd1.92O3 solid solution slightly shift toward large angle side with respect to undoped Gd2O3. NMAT 2020Journal of Physics: Conference Series 1942 (2021) 012026IOP Publishingdoi:10.1088/1742-6596/1942/1/0120264      Figure 2. X-ray diffraction patterns of the as-synthesized and calcined Tm:Gd2O3 nanopowders.  According to our previous works [9,10], rare-earth sesquioxides such as Y2O3 and Lu2O3 synthesized by laser ablation can be fully converted from the metastable monoclinic phase (B-modification) into the cubic phase (C-modification) by calcination at 900–1100 °C. The transformation B→C was observed in Gd2O3 under specific experimental conditions sustaining alternative routes of phase conversion including water, high pressure or starting materials synthesized by uncommon approaches while the opposite conversion C→B is occurred at a temperature of about 1200 °C [11-14].This may mean that in the case of Gd2O3 the cubic structure is metastable rather than the monoclinic one. This fact predetermined the impossibility of fabricating highly transparent ceramics from the synthesized batch of Tm:Gd2O3 nanopowder since the refractive index of such polycrystalline material will be anisotropic leading to light scattering at the grain boundaries due to a different crystallographic orientation of each grain. This problem can be solved by achievement of an amorphous state of synthesized particles by reducing their characteristic sizes down to ~5 nm with the subsequent transformation into the cubic modification during heat treatment [15]. Particle size of laser-ablated nanopowders can be controlled by increasing the velocity of buffer gas or decreasing the pressure in the evaporation chamber, which requires additional investigations.   NMAT 2020Journal of Physics: Conference Series 1942 (2021) 012026IOP Publishingdoi:10.1088/1742-6596/1942/1/0120265      Table 1. X-ray diffraction data of Tm:Gd2O3 nanoparticles before and after calcination. Heat treatment Crystalline phases Lattice parametersa – Solid solution of Tm2O3 in Gd2O3 with monoclinic phase, space group C2/m a=14.095 Å; b=3.571 Å; c=8.758 Å; β=100.182 °; CSR=23 nm; ρ=8.35 g/cm3 900 °C / 3 h a=14.091 Å; b=3.570 Å; c=8.758 Å; β=100.182 °; CSR=53 nm; ρ=8.35 g/cm3 1100 °C / 3 h a=14.087 Å; b=3.570 Å; c=8.756 Å; β=99.99 °; CSR=70 nm; ρ=8.41 g/cm3 1200 °C / 3 h a=14.079 Å; b=3.571 Å; c=8.752 Å; β=99.99 °;  CSR=150 nm; ρ=8.36 g/cm3 a CSR – coherent scattering region.  The dependences of linear shrinkage and shrinkage rate on temperature for compacts prepared from laser-ablated Tm:Gd2O3 nanoparticles and micro-sized Gd2O3 powder are presented in Figure 3. A sharp decrease in the linear dimensions of the Gd2O3 sample (Fig. 3b) starts at 750 °C and the maximum shrinkage rate is realized at 1290 °C where the shrinkage is -8.1%. A noticeable change in the linear size in the vicinity of this temperature is associated with a stepwise increase in the density of compact due to the phase transformation of the Gd2O3 micro-sized powder from C-modification (ρ=7.41 g/cm3) to B-modification (ρ=8.35 g/cm3). On the shrinkage curve, this process appears as an abrupt dip. In turn, for laser-ablated Tm:Gd2O3 nanoparticles, such phenomena are not observed (Fig. 3a) confirming the absence of any phase transformations with an increase in temperature. Densification of nano-sized particles starts at ~250 °С, much earlier than in the previous case and almost completely ends at around 1150 °C. The maximum change in linear dimensions is -28.2%, which is more than 3 times higher than the similar parameter for micro-sized particles. Figure 3. Densification behaviour of powder compacts prepared from laser ablated Tm:Gd2O3 nanoparticles (a) and commercial Gd2O3 powder with micro-sized particles (b). 4. Conclusion Nano-sized particles of Tm0.08Gd1.92O3 solid solution with the monoclinic phase were synthesized by laser ablation of solid target. Unlike Y2O3 and Lu2O3, transformation of the monoclinic phase into the cubic phase was not observed in laser-ablated Tm:Gd2O3 nanoparticles upon calcination at a temperature of 1200 °C. Nevertheless, the as-synthesized nanopowder exhibited high sinterability with respect to micro-sized particles and the value of linear shrinkage reached as high as -27.4% at 1150 °C corresponding to a relative density of about 89.2%. Thus, the obtained results indicate that the fabrication of highly transparent Tm:Gd2O3 ceramics with cubic structure would require to develop a productive method for the synthesis of ultrafine (~5 nm) nanoparticles in amorphous state. NMAT 2020Journal of Physics: Conference Series 1942 (2021) 012026IOP Publishingdoi:10.1088/1742-6596/1942/1/0120266      Acknowledgements The reported study was funded by RFBR and Sverdlovsk region, project number 20-48-660039. References [1] Krankel C 2015 IEEE J. Sel. Top. Quantum Electron. 21 1602013. [2] Abrashev M V, Todorov N D, and Geshev J 2014 J. Appl. Phys. 116 103508. [3] Goldstein A, Goldenberg A, and Hefetz M 2009 J. Ceram. Soc. Jpn. 117 1281. [4] Krell A, Hutzler T, Klimke J, and Potthoff A 2010 J. Am. Ceram. Soc. 93 2656. [5] Zhang H, Kim B.-N, Morita K, Yoshida H, Hiraga K, and Sakka Y 2011 J. Am. Ceram. Soc. 94 3206. [6] Sokol M, Kalabukhov S, Kasiyan V, Dariel M P, and Frage N 2016 J. Am. Ceram. Soc. 99 802. [7] Osipov V V, Shitov V A, Maksimov R N, Lukyashin K E, Solomonov V I, and Ishchenko A V 2019 J. Am. Ceram. Soc. 102 4757. [8] Osipov V V, Platonov V V, Lisenkov V V, Podkin A V, and Zakharova E E 2013 Phys. Status Solidi C 10 926. [9] Bagayev S N, Osipov V V, Solomonov V I, Shitov V A, Maksimov R N, Lukyashin K E, Vatnik S M, and Vedin I A 2012 Opt. Mater. 34 1482. [10] Maksimov R N, Esposito L, Hostasa J, Shitov V A, and Belov P A 2016 Mat. Lett. 185 396. [11] Roth R S, and Schneider S J 1960 J. Res. Natl. Bur. Stand. A Phys. Chem. 64A 309. [12] Shaffer M W, and Roy R 1959 J. Am. Ceram. Soc. 42 563. [13] Warshaw J, and Roy R 1961 J. Phys. Chem 65 2048. [14] Brauer G, and Muller R 1963 Z. Anorg. Allg. Chem. 321 234. [15] Il’ves V G, Sokovnin S Yu, Uporov S A, and Zuev M G 2013 Phys. Solid State 55 1262. 

Laser Ablation Synthesis and Characteristics of Tm-Doped Gd2O3 Nanoparticles

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Laser Ablation Synthesis and Characteristics of Tm-Doped Gd2O3 Nanoparticles

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