Thermal stability, cation dynamics, and ferroelastic domain walls in the α→β→γ phase transitions of perovskite (C2H5NH3)2MnCl4 crystals

被引:4
作者
Lim, Ae Ran [1 ,2 ]
Kim, Sun Ha [3 ,4 ]
机构
[1] Jeonju Univ, Analyt Lab Adv Ferroelect Crystals, Jeonju 55069, South Korea
[2] Jeonju Univ, Dept Sci Educ, Jeonju 55069, South Korea
[3] Korea Basic Sci Inst, Seoul Western Ctr, Seoul 120140, South Korea
[4] Kyungpook Natl Univ, Dept Chem, Daegu 41566, South Korea
基金
新加坡国家研究基金会;
关键词
C2H5NH3)(2)MnCl4; Phase transition; Thermal stability; Nuclear magnetic resonance; Ferroelastic domain; H-1 MAS NMR; SIDE-BAND; X-RAY; STATE; TETRACHLOROMANGANATE(II); BIREFRINGENCE; BEHAVIOR;
D O I
10.1016/j.solidstatesciences.2020.106365
中图分类号
O61 [无机化学];
学科分类号
070301 ; 081704 ;
摘要
Differential scanning calorimetry (DSC) and thermogravimetric analysis (TGA) confirmed that the (C2H5NH3)(2)MnCl4 crystal undergoes alpha-beta-gamma phase transitions at approximately T-C2 = 225 K and T-C1 = 424 K, remains stable until 470 K, and displays a weight loss of 25.24% at around 579 K due to partial thermal decomposition. Cation dynamics near these temperatures was investigated by MAS H-1 NMR and MAS C-13 NMR experiments. The small changes in the H-1 chemical shift for C2H5 near T-C2 are consistent with the transition from the orthorhombic gamma-phase to the orthorhombic beta-phase. Also, the abrupt changes in NMR signals near T-C1 correspond to structural change from the orthorhombic beta-phase to the tetragonal alpha-phase. The C-13 spin-lattice relaxation time in the rotating frame (T-1 rho) below T-C2 is shorter for CH3 than that for CH2, due to the greater mobility at the free end of the alkyl chain. In addition, the temperature-dependent ferroelastic domain structure was studied near the alpha-beta phase transition. There was no noticeable temperature dependence in H-1 and C-13 T-1 rho values at T-C1 and T-C2, whereas the change in the domain wall was prominent near T-C1.
引用
收藏
页数:6
相关论文
共 31 条
[1]   Effect of organic chain length on structure, electronic composition, lattice potential energy, and optical properties of 2D hybrid perovskites [(NH3)(CH2)n(NH3)]CuCl4, n=2-9 [J].
Abdel-Aal, Seham K. ;
Kocher-Oberlehner, Gudrun ;
Ionov, Andrei ;
Mozhchil, R. N. .
APPLIED PHYSICS A-MATERIALS SCIENCE & PROCESSING, 2017, 123 (08)
[2]   Synthesis, structure, lattice energy and enthalpy of 2D hybrid perovskite [NH3(CH2)4NH3]CoCl4, compared to [NH3(CH2)nNH3]CoCl4, n=3-9 [J].
Abdel-Aal, Seham K. ;
Abdel-Rahman, Ahmed S. .
JOURNAL OF CRYSTAL GROWTH, 2017, 457 :282-288
[3]  
Abragam A., 1961, The principles of nuclear magnetism
[5]   Changing the Usual Interpretation of the Structure and Ground State of Cu2+-Layered Perovskites [J].
Aramburu, J. A. ;
Garcia-Fernandez, P. ;
Mathiesen, N. R. ;
Garcia-Lastra, J. M. ;
Moreno, M. .
JOURNAL OF PHYSICAL CHEMISTRY C, 2018, 122 (09) :5071-5082
[6]   THE LAYERED PEROVSKITES (C3H7NH3)2MNCL4(PAMC), AND (C2H5NH3)2MNCL4(EAMC) - BIREFRINGENCE STUDIES AND THE SYMMETRY OF THE COMMENSURATELY MODULATED EPSILON PHASE OF PAMC [J].
BRUNSKILL, IH ;
DEPMEIER, W .
ACTA CRYSTALLOGRAPHICA SECTION A, 1982, 38 (JAN) :132-137
[7]   X-RAY STUDY OF 1ST-ORDER PHASE-TRANSITION PCAB-BMAB IN (CH3CH2NH3)2CDC14 [J].
CHAPUIS, G .
PHYSICA STATUS SOLIDI A-APPLIED RESEARCH, 1977, 43 (01) :203-212
[8]   X-RAY STUDY OF STRUCTURAL PHASE-TRANSITIONS IN PEROVSKITE-TYPE LAYER COMPOUND (CH3NH3)2CDCL4 [J].
CHAPUIS, G ;
KIND, R ;
AREND, H .
PHYSICA STATUS SOLIDI A-APPLIED RESEARCH, 1976, 36 (01) :285-295
[9]   STRUCTURE OF BETA-BIS(ETHYLAMMONIUM) TETRACHLOROMANGANATE(II) - NEUTRON REFINEMENT [J].
DEPMEIER, W ;
HEGER, G .
ACTA CRYSTALLOGRAPHICA SECTION B-STRUCTURAL SCIENCE, 1978, 34 (MAY) :1698-1700
[10]   PHASES AND PHASE-TRANSITIONS OF COMPOUNDS (CNH2N+1NH3)2MNCL4 WITH N=1,2,3 [J].
DEPMEIER, W ;
FELSCHE, J ;
WILDERMUTH, G .
JOURNAL OF SOLID STATE CHEMISTRY, 1977, 21 (01) :57-65