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1.
Dielectric constant (?) and loss (tan δ) of EuF2 have been measured for the first time as a function of frequency in the temperature range from liquid nitrogen to 300°C. The data has been used to obtain the values of conductivity (σ). The conductivity values are frequency independent in the high temperature region and yield 1.05 eV for the activation energy for conduction.  相似文献   

2.
In the system Li4SiO4-Li3AsO4, Li4SiO4 forms a short range of solid solutions containing up to 14 to 20% Li3AsO 4, depending on temperature, and γ-Li3AsO4 forms a more extensive range of solid solutions containing up to ≈55% Li4SiO4. The Li4SiO4-Li3AsO4 phase diagram has been determined and is of binary eutectic character. The ac conductivity of polycrystalline samples was measured over the range 0 to at least 300°C for nine different compositions. The two solid solution series have much higher conductivity than the pure end-members; maximum conductivity was observed in the γ-Li3AsO4 solid solutions containing ≈40 to 55% Li4SiO4, with values of ≈2×10?6 Ω?1 cm?1 at 20°C rising to ≈0.02 Ω?1 cm?1 at 300°C. These values are comparable to those found in the system Li4SiO4-Li3PO4. The variation with composition of the Arrhenius prefactor and activation energy has been interpreted in terms of the mechanisms of conduction. Li3AsO4 is a poor conductor essentially because the number of mobile Li+ ions is very small. This number, and hence the conductivity, increases dramatically on forming solid solutions with Li4SiO4, by the creation of interstitial Li+ ions. At ≈40 to 55% Li4SiO4, the number of mobile Li+ ions appears to be optimised. An explanation for the change in activation energy of conduction at ≈290°C in Li4SiO4 and at higher temperatures in Li4SiO4 solid solutions is given in terms of order-disorder of the Li+ ions.  相似文献   

3.
The electron concentration and mobility in polycrystalline In2O3 have been measured as a function of temperature and partial oxygen pressure, in the temperature range from 25 to 700°C. These experimental data are critically compared with literature data. A conduction model is proposed. Theoretical values of the electron concentration as a function of the partial oxygen pressure are reported for temperatures from 700 to 1400°C. An estimate is given for the minimum room temperature “intrinsic” electron concentration in In2O3 after a high temperature annealing experiment. It is also shown that interpretations of conductivity values for porous material in terms of carrier concentration only, can be very misguiding.  相似文献   

4.
The d.c. electrical conductivity of pure, doped and quenched samples of LiNH4SO4 is measured between liquid nitrogen temperature and 290°C. A-type conductivity anomalies are observed at 10°C and at 186.5°C along the ferroelectric axis. The mechanisms of electrical conduction in the various phases and at the transition points are discussed.  相似文献   

5.
NH4H2PO4 (ADP) has been investigated by infrared spectroscopy, differential scanning calorimetry, thermogravimetric analysis and d.c. conductivity in the temperature range of 25–180° C. Sharp reversible changes were observed in the region from 400 to 500 cm?1 of the infrared spectra in the temperature range of 138–174° C. Similar and supportive data were obtained with DSC, TGA and DC conductivity measurements. The results clearly suggest a high temperature phase transition for ADP before its melting point.  相似文献   

6.
Taking oxygen ion conductor La2Mo2O9, as a base compound, a series of Sn-doped La2Mo2−x Sn x O9−δ, x = 0, 0.01, 0.02, 0.03, 0.05, 0.1, 0.15, 0.2 specimens were prepared and characterized by XRD for phase and crystal structure determination and ac impedance spectroscopy for ac and dc conductivity measurement. We have found that there is slight improvement in overall conductivity of the specimen with x = 0.03 at 800°C compared to the undoped compound at the same temperature. The value of conductivity when extrapolated to 800°C is found to be 0.055 S cm-1 for the specimen with x = 0.03, whereas conductivity of undoped specimen at the same temperature is found to be 0.033 Scm−1.  相似文献   

7.
Electrical conductivity of the solid system AgI-Sb2S3 and its dependence on composition within the temperature range from room temperature to 280°C was investigated. The temperature of phase transition β→α AgI divides the conductivity region into low-temperature and high-temperature parts. Within the high-temperature region the conductivity increases monotonously with an increase in mole fraction of AgI, while within the low-temperature one its maximum appears at Agl mole fraction of 0.6. This composition is glassy and was investigated in detail with regard to the conductivity and the double layer capacitance. The electric conductivity course was explained in the light of structure investigations.  相似文献   

8.
The ionic and electronic conductivities of the lithium nitride bromides Li6NBr3 and Li1 3N4Br have been studied in the temperature range from 50 to 220°C and 120 to 450°C, respectively. Both compounds are practically pure lithium ion conductors with negligible electronic contribution. Li6NBr3 has an ionic conductivity Ω of 2 × 10-6Ω-1cm-1 at 100°C and an activation enthalpy for σT of 0.46 eV. Li1 3N4Br shows a phase transition at about 230°C. The activation enthalpy for σT is 0.73 eV below and 0.47 eV above this temperature. The conductivities at 150 and 300°C were found to be 3.5 × 10-6 Ω-1cm-1 and 1.4 × 10-3Ω-1cm-1, respectively. The crystal structure is hexagonal at room temperature with a = 7.415 (1)A? and c = 3.865 (1)A?.  相似文献   

9.
The electrical conductivity of the solid phase Na2SO4(I) has been measured between the melting point at 884°C and the first order phase transition at about 240°C. The measurements have been performed using complex impedance measurements on pellet samples as well as on U-cells. The electrical conductivity is strongly dependent on sample at low temperatures and the activation energy ranges from 0.5 eV to 1.7 eV over the measured temperature range.  相似文献   

10.
Careful axiswise measurements of d.c. conductivity and dielectric constants of (NH4)2SO4 from 50 to - 196°C establish two distinct phase transitions, instead of one, at temperatures -49.5 and -58°C which remain unchanged in (ND4)2SO4. Explanation based on successive distortions of non-equivalent (NH4)+ is offered. Low temperature transport process in the crystal also is discussed.  相似文献   

11.
Mixtures of AgI and PbI2 cooled from the melt result in the peritectic formation of a fast ion conducting phase centred about Ag4PbI6, which is face centred cubic with a = 6.33(5)A; this phase exhibits high electrical conductivity. On cooling to about 125°C, dissociation occurs to γAgI and PbI2, accompanied by the transient formation of another phase, centred about Ag2PbI4. A modified form of the T-x section of the equilibrium phase diagram at AgI concentrations greater than 60 mole % and below 300°C is proposed.  相似文献   

12.
Improvement of low-temperature performance of oxygen sensor was studied by preparing a thin film of 15 μm thickness. Melt-quenched Bi2O3 film doped with 16 mol% MoO3 was used as an electrolyte after HF treatment. Impedance measurements were carried out in the frequency range DC-100 KHz. Resistance of electrolyte in the form of thin film (110ω) was negligibly small compared with the overall resistance of the cell (287 Kω) at 350°C. Oxygen/air concentration cell was constructed and the cell performance was measured at 350 and 300°C. Transference number close to unity and rapid response were observed at 350°C, however the cell showed a long response time of about 3 min at 300°C.  相似文献   

13.
The ionic conduction of sintered samples of Bi2O3?Y2O3 containing 20–30 mol% Y2O3 has been investigated by means of ac conductivity experiments and EMF measurement of an oxygen concentration cell using the specimen tablet as electrolyte. Ac conductivity was measured at a frequency of 10 kHz under oxygen partial pressures ranging from 1 to 10-21 atm. The results show that these materials possess high ionic conduction. The conductivities for samples containing 22.5–30 mol% Y2O3 are many times higher than those of stabilized zirconia-based solid electrolyte at corresponding temperatures. The ratio of Emeas./Ecalc. of an oxygen concentration cell Pt∣O2(air)∣Bi2O3?Y2O3∣O2(pure oxygen)∣Pt is close to 1 which shows that the materials containing 22.5 to 30 mol% Y2O3 are nearly pure ionic conductors. The p-type conductivity is negligible at higher PO2 values. The n-type conduction for a sample containing 27.5 mol% Y2O3 was investigated using the Coulomb titration technique in which the following cell was used: Pt Rh∣O2(air)∣Bi2O3?Y2O3∣[O]sn∣W.log Pé=-767000/T+665. Pé is equal to 2.6×10-61 atm at 800°C. The n-type conductivity is also very small. Thus these materials are good oxygen ionic conductors.  相似文献   

14.
Single phase of Li3AlN2 was prepared from the mixture of Li3N/AlN = 1.2 to 1.5 in molar ratio at 700°C and at 900°C. It crystalizes in the cubic system derived from antifluorite-type structure having the lattice parameter a = 9.470 A?. It is a pure ionic conductor having conductivity of 5 × 10?8ω?1cm?1 at room temperature and an activation energy of 52 kJ/ mol. Its decomposition voltage was 0.85 V at 104°C. The TiS2/Li3AlN2/Li cell could be discharged at a constant current of 45 μA/cm2 at 104°C.  相似文献   

15.
Measurements of dc conductivity and dielectric constant show that deuteration causes an upward shift of the high temperature phase transition point from 186.5 to 191°C and a downward shift of the low temperature transition point from 10 to -1.5°C in LiNH4SO4. Mechanisms of phase transitions and of electrical transport in the crystal are discussed.  相似文献   

16.
本文采用化学湿磨法,首次将金属氧化物Mn3O4包覆于LiNi0.5Mn1.5O4颗粒表面,使得电极材料的电子电导率从1.53×10-7 S/cm 提高到3.15×10-5 S/cm. 电化学测试结果表明Mn3O4包覆大大提高LiNi0.5Mn1.5O4正极材料的倍率性能和高温循环稳定性. 最佳包覆样品为2.6wt% Mn3O4包覆的LiNi0.5Mn1.5O4,在10 C倍率下具有108 mAh/g的高放电容并且在55 °C下100次循环后仍有78%的容量保持率,远大于未包覆样品67%的容量保持率.  相似文献   

17.
We have measured the effect of varying the mobile ion concentration on the sodium ion conductivity in the Hf-Nasicon system, Na1+xHf2SixP3-xO12, for 1.4 ? x ? 2.8. The conductivity is greatest for Na3.2Hf2Si2.2 P0.8O12: σ25°C = 2.3 × 10?3 (ω cm)?1, and σ250°C = 1.7 × 10?1 (ω cm)?1. These values are approximately 50% greater and worse, respectively, than the values reported for the best Zr-Nasicon. We have characterized the variation of lattice parameters with composition and found the behavior to be similar to that of Zr-Nasicon. A small distortion from rhombohedral to monoclinic symmetry occurs for compositions 1.8 ? x ? 2.2.  相似文献   

18.
A new compound, Na4ZrSi3O10, belonging to the ternary system Na2O-SiO2-ZrO2 is presented. Based on X-ray powder methods, it is assigned monoclinic symmetry with the probable group C 2/c. The ionic conductivity was found to be 4 x 10-3Ω-1cm-1 at 300°C and the activation energy for ionic motion is 42 kJ/mol.  相似文献   

19.
The appearance of a “liquid-like” proton T2 component above 100°C and the relatively high value of the proton self-diffusion coefficient D = (5–8) × 10-7cm2sec-1 between 175°C and 200°C demonstrate the onset of a super-ionic state in N(CH3)4HSO4. The ratio between the “liquid” and “solid” like components shows that acid protons are responsible for the high ionic conductivity.  相似文献   

20.
Attempts have been made to synthesize a few compositions Ce0.80La0.15Al0.05O1.90, Ce0.80Sm0.10Gd0.05Al0.05O1.90, and Ce0.80Gd0.10Sm0.05Al0.05O1.90 by citrate–nitrate auto-combustion method. The aim of the present investigation was to study the effect of co-doping and multiple doping on the ionic conductivity of CeO2 for its use as solid electrolyte in intermediate temperature solid oxide fuel cells. XRD patterns showed that all the samples have fluorite-type crystal structure similar to undoped ceria. Microstructures of thermally etched samples have been studied by scanning electron microscopy. Contributions of grains σ g and grain boundaries σ gb to the total conductivity σ T, have been determined using impedance analysis. Impedance measurements were made in the frequency range 1 Hz–1 MHz and temperature range 250–500 °C. Our experimental results show that multiple doping is more effective than co-doping for improving the oxide ion conductivity of ceria in the materials investigated in the present study.  相似文献   

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