Ferroelectric to paraelectric structural transition in LiTaO3 and LiNbO3

被引:3
|
作者
Bernhardt, Felix [1 ,2 ]
Verhoff, Leonard M. [1 ]
Schaefer, Nils A. [1 ]
Kapp, Alexander [1 ]
Fink, Christa [1 ,2 ]
Al Nachwati, Wafaa [1 ]
Bashir, Umar [3 ]
Klimm, Detlef [3 ]
El Azzouzi, Fatima [4 ]
Yakhnevych, Uliana [4 ]
Suhak, Yuriy [4 ]
Schmidt, Harald [5 ]
Becker, Klaus -Dieter [6 ]
Ganschow, Steffen [3 ]
Fritze, Holger [4 ]
Sanna, Simone [1 ,2 ]
机构
[1] Justus Liebig Univ Giessen, Inst Theoret Phys, Heinrich Buff Ring 16, D-35392 Giessen, Germany
[2] Justus Liebig Univ Giessen, Ctr Mat Res ZfM LaMa, Heinrich Buff Ring 16, D-35392 Giessen, Germany
[3] Leibniz Inst Kristallzuchtung, Max Born Str 2, D-12489 Berlin, Germany
[4] Tech Univ Clausthal, Inst Energieforsch & Phys Technol, Stollen 19B, D-38640 Goslar, Germany
[5] Tech Univ Clausthal, Inst Met, D-38678 Clausthal Zellerfeld, Germany
[6] Tech Univ Carolo Wilhelmina Braunschweig, Inst Phys & Theoret Chem, D-38106 Braunschweig, Germany
来源
PHYSICAL REVIEW MATERIALS | 2024年 / 8卷 / 05期
关键词
OPTICAL-DAMAGE RESISTANCE; TOTAL-ENERGY CALCULATIONS; MOLECULAR-DYNAMICS; LITHIUM-NIOBATE; TEMPERATURE-DEPENDENCE; PHASE-TRANSITION; POLARIZATION; RAMAN; ASSIGNMENT; SCATTERING;
D O I
10.1103/PhysRevMaterials.8.054406
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
The ferroelectric to paraelectric phase transition in LiTaO 3 and in pure as well as Mg -doped LiNbO 3 is investigated theoretically by atomistic calculations in the framework of the density functional theory, as well as experimentally by calorimetry and electrical conductivity measurements. First -principles models within the stochastic self -consistent harmonic approximation (SSCHA) allow to consider anharmonic effects and thus to obtain a realistic estimate of the Curie temperature T C of both ferroelectrics. Ab initio molecular dynamics (AIMD) calculations performed on large supercells confirm the Curie temperatures estimated with the SSCHA approach. Moreover, they also suggest that the structural phase transition is a continuous process beginning at temperatures well below T C . According to AIMD, significant ionic displacements occur already at temperatures of about 100 K and 300 K below T C in LiTaO 3 and LiNbO 3 , respectively. To asses whether and how far the ionic displacements affect the materials properties, the AIMD results are compared with measurements of the electrical conductivity and of the heat capacity across the phase transition. Our first -principles calculations moreover show that Mg ions, a frequently employed dopant, raise the Curie temperature in LiNbO 3 .
引用
收藏
页数:14
相关论文
共 50 条
  • [31] Electric field gradients at the 111In site in the ferroelectric and paraelectric phases of LiTaO3
    J.G. Marques
    A. Kling
    C.M. de Jesus
    J.C. Soares
    P. Friedsam
    K. Freitag
    R. Vianden
    Hyperfine Interactions, 1999, 120-121 : 485 - 489
  • [32] Ferroelectric phase transition in LiNbO3: insights from molecular dynamics
    Sanna, Simone
    Schmidt, Wolf Gero
    2011 INTERNATIONAL SYMPOSIUM ON APPLICATIONS OF FERROELECTRICS (ISAF/PFM) AND 2011 INTERNATIONAL SYMPOSIUM ON PIEZORESPONSE FORCE MICROSCOPY AND NANOSCALE PHENOMENA IN POLAR MATERIALS, 2011,
  • [33] Origin of the difference in thermal conductivity and anharmonic phonon scattering between LiNbO3 and LiTaO3
    Fu, Yangbin
    Wei, Hui
    Wei, Lei
    Zhang, Huadi
    Wang, Xuping
    Liu, Bing
    Zhang, Yuanyuan
    Lv, Xianshun
    Zhou, Jixue
    Yu, Huajian
    CRYSTENGCOMM, 2021, 23 (48) : 8572 - 8578
  • [34] Proton exchanged waveguides in LiNbO3 and LiTaO3 for integrated lasers and nonlinear frequency converters
    Baldi, P
    De Micheli, MP
    El Hadi, K
    Nouh, S
    Cino, AC
    Aschieri, P
    Ostrowsky, DB
    OPTICAL ENGINEERING, 1998, 37 (04) : 1193 - 1202
  • [35] Investigation of the piezoelectric effect in LiNbO3 and LiTaO3 crystals by X-ray diffraction
    Irzhak, Dmitry
    Roshchupkin, Dmitry
    Punegov, Dmitry
    FERROELECTRICS, 2007, 351 : 163 - 175
  • [36] Investigations of LiNbO3 and LiTaO3 single crystals for pyroelectric applications in the wide temperature range
    Bravina, S. L.
    Morozovsky, N. V.
    Morozovska, A. N.
    Gille, S.
    Salvestrini, J.-P.
    Fontana, M. D.
    FERROELECTRICS, 2007, 353 : 636 - 645
  • [37] Nonlinear optical properties of different types of proton exchanged LiNbO3 and LiTaO3 waveguides
    Korkishko, YN
    Fedorov, VA
    Kostritskii, SM
    Alkaev, AN
    Maslennikov, EI
    Laurell, F
    INTEGRATED OPTICAL DEVICES: FABRICATION AND TESTING, 2002, 4944 : 268 - 279
  • [38] Multiphoton photoluminescence contrast in switched Mg:LiNbO3 and Mg:LiTaO3 single crystals
    Reichenbach, P.
    Kaempfe, T.
    Thiessen, A.
    Haussmann, A.
    Woike, T.
    Eng, L. M.
    APPLIED PHYSICS LETTERS, 2014, 105 (12)
  • [39] Multicycle terahertz pulse generation by optical rectification in LiNbO3, LiTaO3, and BBO crystals
    Jang, Dogeun
    Kim, Ki-Yong
    OPTICS EXPRESS, 2020, 28 (14): : 21220 - 21235
  • [40] Electrostatic Model of the LiTaO3 Ferroelectric
    Yatsenko, A. V.
    CRYSTALLOGRAPHY REPORTS, 2017, 62 (01) : 118 - 122