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Study On The Structural And Electrical Properties Of ABO4 Tungstates And Molybdate Under High Pressure

Posted on:2018-01-30Degree:DoctorType:Dissertation
Country:ChinaCandidate:L WanFull Text:PDF
GTID:1310330515474254Subject:Condensed matter physics
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ABO4 compounds are common accessory minerals on the earth and important functional materials.The studies of ABO4 compounds under high pressure are helpful for understanding the physical and chemical properties of these minerals and improving their physical and mechanical properties.Tungstates and molybdates are typical ABO4 compounds.Especially,the scheelite is also a high-pressure phase of other ABO4 compounds?e.g.zircon,monazite and Cr VO4-type compounds?.So,the study on scheelite at high pressures will provide significant reference for exploring the high-pressure behaviors of other ABO4 compounds.In this thesis,by combining the high-pressure synchrotron X-ray diffraction,alternating current impedance spectra measurements and first-principles calculations,we have studied systematically the high-pressure structural and electrical transport properties of ABO4 tungstates and molybdate,including scheelite-structured Ca WO4,Ca Mo O4,Sr WO4,wolframite-structured Mg WO4,and distorted wolframite-structured Cu WO4.The results of study are as follows:1.By combining first-principles structure prediction and X-ray diffraction measurements,we found that Ca WO4 transformed from tetragonal scheelite structure?I41/a?to monoclinic fergusonite structure?I2/a?at 10.0 GPa,and then to layered monoclinic structure?P21/m?at 38.0 GPa.These two phase transitions are secondand first-order phase transitions,respectively.In I41/a phase,Ca WO4 compresses anisotropically with c > a.In I2/a phase,the unit-cell parameter of Ca WO4 shows a strong non-linear behavior.Besides,we found that the P21/m phase of Ca WO4 has a smaller band gap than the other two phases.By alternating current impedance spectra measurements,we found that the pressure-induced structural phase transitions significantly change the electronic structure of Ca WO4 that gives rise to abnormal variations in electrical transport properties.Besides,we found a monoclinic structure?P21/c?with the lowest energy and we attribute this structure to a high-temperature high-pressure phase.This work observes the I2/a ? P21/m phase transition for the first time in the X-ray diffraction experiment and enriches the information of ABO4 compounds under high pressure.It is an important reference for the high-pressure research of other ABO4 compounds.2.Ca Mo O4 displays similar behaviors with Ca WO4 under high pressure.Ca Mo O4 undergoes a second-order structural phase transition from tetragonal scheelite structure?I41/a?to monoclinic fergusonite structure?I2/a?around 10.0 GPa.The second structural phase transition occurs at a pressure of 42.1 GPa,changing the space group from I2/a to P21/m.Under high pressure,in I41/a phase,compression is anisotropic,being the c-axis more compressible than the a-axis.The unit-cell parameter of I2/a phase shows a non-linear change.In addition,we calculated the electronic band structures under different pressures.The results show that the I41/a,I2/a,and P21/m phases are direct bandgap semiconductor,direct bandgap semiconductor,and indirect bandgap semiconductor,respectively.The bandgap of Ca Mo O4 decreases with increasing pressure.These results will be significant for further understanding the physical properties of ABO4 compounds at high pressures.3.The phase-transition sequence of Sr WO4 at high pressures is quite different from those of Ca WO4 and Ca Mo O4.In Sr WO4 a phase transition from tetragonal scheelite structure?I41/a?to monoclinic fergusonite structure?I2/a?was found at 9.1 GPa.The second structural phase transition takes place at 12.3 GPa.By combining theory with experiment,the high-pressure new phase is defined to have an orthorhombic structure?Cmca?,rather than decomposition as reported in previous study.Meanwhile,the structural phase transitions give rise to abnormal variations in bandgap and electrical transport parameters.In all structures,the resistance of Sr WO4 decreases with increasing pressure.All the activation energies decrease with increasing pressure and the charge-discharge process becomes easier.This work for the first time prove the prediction from the experiment that the scheelite structure can transform to the Cmca structure at high pressures.4.In Mg WO4,we found two phase transitions at 17.2 GPa and 37.0 GPa,respectively.The first phase transition is from monoclinic wolframite structure?P2/c?to triclinic Cu WO4 structure?P-1?and the second one is to an unknown high-pressure phase.At pressures below 16.1 GPa,in monoclinic wolframite structure,Mg WO4 compresses anisotropically with b > a > c.The electrical transport parameters of Mg WO4 vary anormalously along with the structural transitions.At pressures below 16.1 GPa,the band gap becomes larger and the resistance increases slowly with increasing pressure.However,at the first phase transition pressure,the resistance decreases five orders of magnitude that may give rise to narrower bandgap.In P-1 phase,the activation energy decreases with increasing pressure and the charge-discharge process becomes easier.In new high-pressure phase,the activation energy increases with increasing pressure and the charge-discharge process becomes more difficult.5.The effect of crystallization water on the structural and electrical properties of Cu WO4 under high pressure has been investigated by X-ray diffraction and alternating current impedance spectra measurements.The crystallization water was found to be a key role in modulating the structural stability of Cu WO4 at high pressures.The anhydrous Cu WO4 undergoes two pressure-induced structural transitions at 8.8 and 18.5 GPa,respectively,while Cu WO4?2H2O keeps its original structure up to 40.5 GPa.Besides,the crystallization water makes the electrical transport behavior of anhydrous Cu WO4 and Cu WO4?2H2O quite different.The charge carrier transportation is always isotropic in Cu WO4?2H2O,but anisotropic in the triclinic and the third phase of anhydrous Cu WO4.The grain resistance of Cu WO4?2H2O is always larger than that of anhydrous Cu WO4 in the entire pressure range.By analyzing the relaxation response,we found that the large number of hydrogen bonds can soften the grain characteristic frequency of Cu WO4?2H2O over Cu WO4 by one order of magnitude.
Keywords/Search Tags:ABO4, High pressure, Structural transition, Impedance spectra, Crystallization water
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