High Pressure High Temperature Synthesis and Physical Properties of Transition Metal Perovskites
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摘要: 过渡金属钙钛矿材料由于具有灵活多变的晶体结构和丰富多样的物理性质，在信息、能源和催化等领域具有广阔的应用前景。然而，在常规条件下合成的过渡金属钙钛矿种类有限。高压作为一种独特的实验手段，能够显著调控材料的原子间距和元素构型，在合成新型钙钛矿材料方面具有较大优势，通过改变电子结构可引发铁电、磁性、超导、金属-绝缘体转变、电荷转移及电荷歧化等新奇的物理性质。本文回顾了极端高压材料制备技术和高压原位测量技术，并对这2项技术在几类过渡金属钙钛矿合成与物性调控方面的应用进行了展望。Abstract: Transition metal perovskite materials hold broad prospects for applications in fields such as information technology, energy, and catalysis due to their flexible and diverse crystal structures and rich variety of physical properties. However, the types of transition metal perovskite materials synthesized under conventional conditions are limited. High pressure, as a unique experimental approach, can significantly manipulate atomic distances and elemental configurations in materials. This method offers substantial advantages in synthesizing novel perovskite materials and can induce novel physical properties such as ferroelectricity, magnetism, superconductivity, metal-insulator transition, charge transfer and charge disproportionation by altering electronic structures. In this paper, the preparation of extreme high-pressure materials and high-pressure in-situ measurement techniques, as well as their applications in the synthesis and physical properties control of several types of transition metal perovskite materials are reviewed.
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图 1 高压高温合成装置：(a) 活塞圆筒型压机[25]，( b) 六面顶压机[29] ，(c) Kawai型二级增压装置[36]（F为外部压力），(d) Walker型二级增压装置[37] （U为活塞压力），(e) DIA型二级增压装置[38]
Figure 1. High-pressure and high-temperature apparatus: (a) piston-cylinder press[25]; (b) cubic press[29]; (c) Kawai-type muti-anvil module[36] (F being outer force); (d) Walker-type muti-anvil module[37] (U being piston pressure); (c) DIA-type muti-anvil module[38]
图 2 高压原位测量装置：(a) 活塞圆筒压腔[42] ，(b) 立方体压腔[45]，(c) 用于电学测量的金刚石对顶砧[47]，(d) 用于单晶X射线衍射测量的金刚石对顶砧[47]
Figure 2. In-situ high-pressure measurement devices: (a) piston-cylinder cell[42]; (b) cubic anvil cell [45]; (c) diamond anvil cell for electrical measurements[47]; (d) diamond anvil cell for single crystal X-ray diffraction measurements[47]
图 3
1000 t Walker型二级增压装置及校压结果：(a) 6.0 mm切角二级压砧ZnTe的压力-电阻曲线， (b) 2.5 mm切角二级压砧GaAs的压力-电阻曲线，(c) 6.0 mm切角二级压砧校压结果，(d) 2.5 mm切角二级压砧校压结果Figure 3. Pressure calibration of
1000 t Walker-type apparatus: (a) ZnTe resistivity-pressure curve using 6.0 mm edge lengthsecond stage anvil; (b) GaAs resistivity-pressure curve using 2.5 mm edge length second stage anvil; (c) pressure calibration result using 6.0 mm edge length second stage anvil; (d) pressure calibration result using 2.5 mm edge length second stage anvil
图 4 (a) 用于光谱测量的DAC， (b) 用于电磁输运测量的DAC，(c)用于电输运测量的DAC组装示意图
Figure 4. (a) DAC for optic measurements; (b) DAC for electrical and magnetic measurements;(c) electrical measurement assembly in DAC
图 5 钙钛矿及衍生结构：(a)简单钙钛矿的结构畸变，(b)简单钙钛矿的结构单元，(c) A位有序双钙钛矿结构，(d) RP型层状钙钛矿结构
Figure 5. Perovskite and derived structures: (a) structural distortion of simple perovskite; (b) unit cell of simple perovskite; (c) A-site ordered double perovskite; (d) RP-type layered perovskite
图 6 (a) PbVO3的结构畸变和轨道杂化[70]，(b) PbCrO3的复杂晶体结构[71] （其中，黄球为Pb离子，其大小表示填充率高低；紫球为Cr离子；红球为O离子 ），(c) PbMnO3的电荷歧化[75]
Figure 6. (a) Structural distortion and orbital hybridization of PbVO3[70]; (b) complex crystal structure of PbCrO3[71] (Yellow ball is Pb ions, the size of which indicates the filling ratio; purple ball is Cr ions and red ball is O ions.); (c) charge disproportionation of PbMnO3[75]
图 8 (a) ARuO3体系晶体结构示意图[85]，(b) ARuO3体系粉末X射线衍射精修结果[85]，(c) BaRuO3的物性测试结果[85]，(d) Ca/Ba掺杂的SrRuO3体系的结构和物性总结[85]（TG为Griffiths相温度，O代表正交结构，T代表四方结构，C代表立方结构）
Figure 8. (a) Crystal structure of ARuO3 system[85] ; (b) powder XRD refinement result of ARuO3 system[85]; (c) physical properties of BaRuO3[85]; (d) summary of crystal structure and physical properties of Ca/Ba doped SrRuO3 system[85] (TG is Griffiths phase temperature, O stands for orthorhombic structure, T stands for tetragonal structure and C stands for cubic structure.)
图 9 (a) BaIrO3随着压力升高发生的结构转变[91]，(b) 不同结构的BaIrO3的物性演变[91]，(c) BaIrO3的电阻率及磁化率随温度的变化曲线[91]，(d) 不同结构BaIrO3和BaRuO3的磁性[91]
Figure 9. (a) Structural transition of BaIrO3 with increasing pressure[91]; (b) evolution of physical properties of BaIrO3 with various structures[91]; (c) temperature dependent resistivity and magnetic susceptibility of BaIrO3[91]; (d) magnetic susceptibility of BaIrO3 and BaRuO3 polytypes[91]
图 10 (a) NaBF3（B = Mg, Co, Ni, Zn）体系八面体倾角Φ随压力的变化[97] ，(b) NaCoF3的原位高压XRD谱，(c) NaNiF3的原位高压XRD结果[97]（a、b、c为晶格常数）
Figure 10. (a) Pressure dependent of octahedral tilt angle Φ of NaBF3 (B = Mg, Co, Ni, Zn) system[97]; (b) in-situ high pressure XRD patterns of NaCoF3; (c) in-situ high pressure XRD results of NaNiF3[97] (a, b, and c are lattice constants.)
图 12 ACu3Fe4O12体系的新奇物性：(a) CaCu3Fe4O12在高压下的复杂价态和物性转变[111]，(b) SrCu3Fe4O12的新奇离子价态[115]，(c) LaCu3Fe4O12的巨大负热膨胀系数[116]
Figure 12. Novel physical properties of ACu3Fe4O12 system: (a) complex transition of valence state and physical properties of CaCu3Fe4O12 with increasing pressure[111]; (b) strange ironic valence state in LaCu3Fe4O12[115]; (c) giant negative thermal expansion coefficient of SrCu3Fe4O12[116]
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