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Research Article | Open Access

Electrical properties of yttrium calcium oxyborate crystal annealed at high temperature and low oxygen partial pressure

Shiwei TianaLili LiaFeifei ChenaChao JiangaFapeng Yua,( )Yanlu Lia,( )Xiulan DuanaZhengping WangaShujun ZhangbXian Zhaoa
State Key Laboratory of Crystal Materials, Advanced Research Center for Optics of Shandong University, Jinan, 250100, China
ISEM, Australia Institute of Innovative Materials, University of Wollongong, Wollongong, NSW, 2500, Australia

Peer review under responsibility of The Chinese Ceramic Society.

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Abstract

The yttrium calcium oxyborate crystal (YCa4O(BO3)3, YCOB) has been actively studied for high-temperature piezoelectric sensing applications. In this work, the stability of electric properties of YCOB crystal annealed in critical conditions (high-temperatures of 900–1100 ℃ with a low oxygen partial pressure of 4 × 10−6 atm for 24 h) was investigated and the recovery mechanism for the electrical resisitivity, dielectric permittivity and dielectric loss were studied, taking advantage of the X-ray photoelectron spectra and the first principle calculations. The electrical resistivity of the annealed YCOB crystal was slightly decreased when compared to the pristine counterpart, being (2–5) × 107 Ω·cm at 850 ℃. The dielectric permittivity and dielectric loss were found to increase after annealing, showing recoverable behaviours after thermal treatment above 650 ℃ in air. The calculated vacancy formation energy indicates that the oxygen vacancy is the dominant defects in YCOB. The formation of oxygen vacancy weakens the chemical bonding strength between B (Ca or Y) and O atoms, introduces extra donor levels in the band gap, which excites the electrons to conduction band more easily thus enhances the electrical conductivity and dielectric loss. The recovered electrical properties are believed to be associated with the reduced vacancy defects at elevated temperatures in air.

References

[1]

Zhang SJ, Yu FP. Piezoelectric materials for high temperature sensors. J Am Ceram Soc 2011;94:3153–70.

[2]

Zhang SJ, Li F, Yu FP, Jiang XN, Lee HY, Luo J, et al. Recent developments in piezoelectric crystals. J Korean Cera Soc 2018;55:419–39.

[3]

Turner RC, Fuierer PA, Newnham RE, Shrout TR. Materials for high temperature acoustic and vibration sensors: a review. Appl Acoust 1994;41:299–324.

[4]

Zhang SJ, Fei YT, Chai BHT, Frantz E, Snyder DW, Jiang XN, Shrout TR. Characterization of piezoelectric single crystal YCa4O(BO3)3 for high temperature applications. Appl Phys Lett 2008;92:202905.

[5]

Markiewicz E, Pawlaczyk C, Pajaczkowska A, Kls A. Piezoelectric and elastic properties of γ-irradiated gadolinium calcium oxoborate, GdCa4O(BO3)3 single crystal. Ferroelectrics 2009;389:55–62.

[6]

Kumar RA, Dhanasekaran R. Nucl Instrum Methods Phys Res Sect B Beam Interact Mater Atoms 2012;287:109–12.

[7]
Zheng YQ, Tu XN, Chen JJ, Gao P, Shi EW. Piezoelectric acceleration sensors based on LGX and ReCOB crystals for application above 645 ℃. 2013 Joint UFFC. In: EFTF and PFM Symp; 2013. p. 977–9.
[8]

Krempl P, Schleinzer G, Wallnö Fer W. Gallium phosphate, GaPO4: a new piezoelectric crystal material for high-temperature sensorics. Sensor Actuat. A-Phys 1997;61:361–3.

[9]

Worsch PM, Krempl PW, Wallnofer W. GaPO4 crystals for sensor applications, Sensors. Proceedings of IEEEE. Comini, Analytica Chimica Acta 2002;1:589–93.

[10]

Yu FP, Hou S, Zhao X, Zhang SJ. High-temperature piezoelectric crystals ReCa4O(BO3)3: a review. IEEE Trans Ultrason Ferroelectr Freq Control 2014;61:1344–56.

[11]

Yu FP, Zhang SJ, Zhao X, Yuan DR, Wang CM, Shrout TR. Characterization of neodymium calcium oxyborate piezoelectric crystal with monoclinic phase. Cryst Growth Des; 2010. p. 1871–7.

[12]

Yu FP, Zhang SJ, Zhao X, Yuan DR, Wang QM, Shrout TR. High temperature piezoelectric properties of yttrium calcium oxyborate single crystals. Phys Stat Solidi RRL 2010;4:103–5.

[13]

Schulz M, Sauerwald J, Richter D, Fritze H. Electromechanical properties and defect chemistry of high-temperature piezoelectric materials. Ionics 2009;15:157–61.

[14]

Damjanovic D. Materials for high temperature piezoelectric transducers. Curr Opin Solid St M 1998;3:469–73.

[15]

Fritze H, Seh H, Tuller HL, Borchardt G. Operation limits of langasite high temperature nanobalances. J Eur Ceram Soc 2001;21:1473–7.

[16]

Fritze H. High temperature bulk acoustic wave sensors. Meas Sci Technol 2010;22:012002.

[17]

Zhang SJ, Zheng YQ, Kong HK, Xin J, Frantz E, Shrout TR. Characterization of high temperature piezoelectric crystals with an ordered langasite structure. J Appl Phys 2009;105:114107.

[18]

Kim T, Kim J, Dalmau R, Schlesser R, Preble E, Jiang XN. High-Temperature electromechanical characterization of AlN single crystals. IEEE Trans Ultrason Ferroelectr Freq Control 2015;62:1880–7.

[19]

Kim K, Zhang SJ, Huang WB, Yu FP, Jiang XN. YCa4O(BO3)3 (YCOB) high temperature vibration sensor. J Appl Phys 2011;109:126103.

[20]

Hou S, Yu FP, Liu YQ, Zhang SJ, Lu QM, Wang SL, et al. Crystal growth and characterization of thulium calcium oxyborate high-temperature piezoelectric crystals. CrystEngComm 2015;17:553–60.

[21]

Zhang SJ, Jiang XN, Lapsley M, Moses P, Shrout TR. Piezoelectric accelerometers for ultrahigh temperature application. Appl Phys Lett 2010;96:013506.

[22]

Zhang SJ, Fei YT, Frantz E, Snyder DW, Chai BHT, Shrout TR. High-temperature piezoelectric single crystal ReCa4O(BO3)3 for sensor applications. IEEE Trans Ultrason Ferroelectr Freq Control 2008;55:2703–8.

[23]

Zu HF, Wu HY, Wang QM. High-temperature piezoelectric crystals for acoustic wave sensor applications. IEEE Trans Ultrason Ferroelectr Freq Control 2016;63:486–505.

[24]

Salazar G, Kim K, Zhang SJ, Jiang XN. Piezoelectric accelerometer for high temperature (1300℃) sensing. Proc SPIE 2011;8347:83471K.

[25]

Johnson JA, Kim K, Zhang SJ, Wu D, Jiang XN. High-temperature acoustic emission sensing tests using a yttrium calcium oxyborate sensor. IEEE Trans Ultrason Ferroelectr Freq Control 2011;61:805–14.

[26]

Jiang XN, Kim K, Zhang SJ, Johnson J, Salazar G. High-temperature piezoelectric sensing. Sensors 2014;14:144–69.

[27]

Norrestam R, Nygren M, Bovin JO. Structural investigations of new calcium-Rare earth (R) oxyborates with the composition Ca4RO(BO3)3. Chem Mater 1992;4:737–43.

[28]

Ilyukhin AB, Dzhurinskii BF. Crystal structures of binary oxoborates LnCa4O(BO3)3 (Ln: Gd, Tb, and Lu) and Eu2CaO(BO3)2. Russ J Inorg Chem 1993;38:847–50.

[29]

Yu FP, Zhang SJ, Zhao X, Guo SY, Duan XL, Yuan DR, et al. Investigation of the dielectric and piezoelectric properties of ReCa4O(BO3)3 crystals. J Phys D Appl Phys 2011;44:135405.

[30]

Kresse G, Furthmuller J. Efficiency of ab-initio total energy calculations for metals and semiconductors using a plane-wave basis set. Comput Mater Sci 1996:615–50.

[31]

Kresse G, Furthmuller J. Efficient iterative schemes for ab initio total-energy calculations using a plane-wave basis set. Phys Rev B 1996;54:11169–86.

[32]

Kresse G, Joubert D. From ultrasoft pseudopotentials to the projector augmented-wave method. Phys Rev B 1999;59:1758–75.

[33]

Ceperley DM, Alder BJ. Ground-state of the electron-gas by a stochastic method. Phys Rev Lett 1980;45:566–9.

[34]

Perdew JP, Zunger A. Self-Interaction correction to density-functional approximations for many-electron systems. Phys Rev B 1981;23:5048–79.

[35]

Monkhorst HJ, Pack JD. Special point for brillouin-zone integrations. Phys Rev B 1976;13:5188–92.

[36]

Mayeshiba T, Morgan D. Strain effects on oxygen vacancy formation energy in perovskites. Solid State Ionics 2017;311:105–17.

[37]

Zhang SJ, Zheng YQ, Kong HK, Xin J, Frantz E, Shrout TR. Characterization of high temperature piezoelectric crystals with an ordered langasite structure. J Appl Phys 2009;105:114107.

[38]

Xia HR, Wang CJ, Yu H, Chen HC, Wang M. Polarization and dipole moments of Co-doped potassium sodium strontium barium niobate crystals. J Appl Phys 1997;82:4465–8.

[39]

Lu GW, Li CX, Wang WC, Wang ZH, Xia HR, Zhang HJ, et al. Lattice vibration and absorbance of Er: Yb: YCOB single crystals. Chem Phys Lett 2003;368:269–75.

[40]

Wu XM, Yu JY, Ren TL, Liu LT. Micro-Raman spectroscopy measurement of stress in silicon. Microelectron J 2007;38:87–90.

[41]

Monteseguro V, Hernandez PR, Vilaplana R, Manjon FJ, Venkatramu V, Errandonea D, et al. Lattice dynamics study of nanocrystalline yttrium gallium garnet at high pressure. J Phys Chem C 2014;118:13177–85.

[42]

Atuchin VV, Kesler VG, Meng G, Lin ZS. The electronic structure of RbTiOPO4 and the effects of the A-site cation substitution in KTiOPO4-family crystals. J Phys Condens Matter 2012;24:1–6.

[43]

Atuchin VV, Pokrovsky LD, Kesler VG, Maklakova NY, Voronkova VI, Yanovskii VK. Superstructure formation and X-ray photoemission properties of the TlTiOPO4 surface. Surf Rev Lett 2004;11:191–8.

[44]

Liu J, Duan XL, Zhang Y, Li ZQ, Yu FP, Jiang HD. Growth, electronic structure and properties of Rb2Ti1.95Yb0.05(PO4)3 crystals. J Alloy Comp 2016;660:356–60.

[45]

Bagusa S, Illas F, Pacchioni G, Parmigiani F. Mechanisms responsible for chemical shifts of core-level binding energies and their relationship to chemical bonding. J Electron Spectrosc 1999;100:215–36.

[46]

Atuchin VV, Kesler VG, Pervukhina NV, Zhang ZM. Ti 2p and O 1s core levels and chemical bonding in titanium-bearing oxides. J Electron Spectrosc 2006;152:18–24.

[47]

Tian SW, Li LL, Yu FP, Li YL, Chen FF, Duan XL, et al. Structural stability and electro-elastic property of YCOB crystal annealed in harsh environment. Appl Phys Lett 2018;113:122905.

[48]

Fukushima K, Adachi H, Imoto S. Electronic state of helium atoms in nickel metal. J Nucl Mater 1986;140:106–12.

Journal of Materiomics
Pages 363-371
Cite this article:
Tian S, Li L, Chen F, et al. Electrical properties of yttrium calcium oxyborate crystal annealed at high temperature and low oxygen partial pressure. Journal of Materiomics, 2019, 5(3): 363-371. https://doi.org/10.1016/j.jmat.2019.02.007

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Received: 11 December 2018
Revised: 26 January 2019
Accepted: 12 February 2019
Published: 13 February 2019
© 2019 The Chinese Ceramic Society. Production and hosting by Elsevier B.V.

This is an open access article under the CC BY-NC-ND license (http://creativecommons.org/licenses/by-nc-nd/4.0/).

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