Stoichiometric Ba（MnxTi（1-x）O3） （BMT） thin films with various values of x were deposited on Si（111） substrates by the sol-gel technique. The influence of Mn content on the optical properties was studied by spe...Stoichiometric Ba（MnxTi（1-x）O3） （BMT） thin films with various values of x were deposited on Si（111） substrates by the sol-gel technique. The influence of Mn content on the optical properties was studied by spectroscopic ellipsometry （SE） in the UV–Vis–NIR region. By fitting the measured ellipsometric parameter （Ψ and Δ） with a four-phase model （air/BMT＋voids/BMT/Si（111））, the key optical constants of the thin films have been obtained. It was found that the refractive index n and the extinction coefficient k increase with increasing Mn content due to the increase in the packing density. Furthermore, a strong dependence of the optical band gap Eg on Mn/Ti ratios in the deposited films was observed, and it was inferred that the energy level of conduction bands decreases with increasing Mn content.展开更多
Raman and IR spectra of Nb-doped PTC Ba1-xPbxTiO3 semiconducting ceramics (x = 0,0. 28,0. 296,0. 313,0. 330,0. 370) have been measured, and mode assignments of Raman scattering frequencies and infrared absorption peak...Raman and IR spectra of Nb-doped PTC Ba1-xPbxTiO3 semiconducting ceramics (x = 0,0. 28,0. 296,0. 313,0. 330,0. 370) have been measured, and mode assignments of Raman scattering frequencies and infrared absorption peaks have been made at room temperature. The influence of Pb2+ ions content on resistivity temperature characteristics and vibration spectra for the Ea1-xPbxTiO3, ceramics have been discussed,and the temperature dependence of the Raman spectra in tetragonal and cubic phases have been investigated from 25 to 340℃. The results indicated that the Raman spectra of the paraelectric phase above Curie point are obviously different from that of ferroelectric phase below Curie point are obviously different from that of ferroelectric phase below Curie point for all the samples. Curie point of each sample,which is determined by resistivity-temperature characteristic measurment, is in good agreement with the results of Raman analysis. The ferroelectric phase transition in the PTCR Bai-xPbxTiO3 ceramics belongs to a distortion or displacement transition.展开更多
Tunable and switchable Ba 0.5 Sr 0.5 TiO 3 film bulk acoustic resonators（FBARs） based on SiO 2 /Mo Bragg reflectors are explored,which can withstand high temperature for the deposition of Ba x Sr 1 x TiO 3（BST） fi...Tunable and switchable Ba 0.5 Sr 0.5 TiO 3 film bulk acoustic resonators（FBARs） based on SiO 2 /Mo Bragg reflectors are explored,which can withstand high temperature for the deposition of Ba x Sr 1 x TiO 3（BST） films at 800 C.The dc bias-dependent resonance may be attributed to the piezoelectricity of the BST film induced by an electrostrictive effect.The series resonant frequency is strongly dc bias-dependent and shifts downwards with dc bias increasing,while the parallel resonant frequency is only weakly dc bias-dependent and slightly shifts upwards at low dc bias（ 45 V） while downwards at higher dc bias.The calculated relative tunability of shifts at series resonance frequency is around 2.3% and the electromechanical coupling coefficient is up to approximately 8.09% at 60-V dc bias,which can be comparable to AlN FBARs.This suggests that a high-quality tunable BST FBAR device can be achieved through the use of molybdenum（Mo） as the high acoustic impedance layer in a Bragg reflector,which not only provides excellent acoustic isolation from the substrate,but also improves the crystallinity of BST films withstanding higher deposition temperature.展开更多
The development of superconductor/insulator/superconductor（SIS）tunnel junctions inthe cuprate high-temperature superconductor family has been hampered by an anisotropicstructure and a coherence length ξ as short as...The development of superconductor/insulator/superconductor（SIS）tunnel junctions inthe cuprate high-temperature superconductor family has been hampered by an anisotropicstructure and a coherence length ξ as short as 0.3 nm. However, the discovery of Ba<sub>1-x</sub>K<sub>x</sub>-BiO<sub>3</sub>（x≈0.4） superconductor which is an isotropic cubic structure and has a展开更多
基金Project supported by the National Natural Science Foundation of China(Grant No.60976016)the Postdoctoral Science Foundation of China(Grant No.2012M511250)the Foundation Co-established by Henan Province and the Ministry of Henan University,China(Grant No.SBGJ090503)
文摘Stoichiometric Ba（MnxTi（1-x）O3） （BMT） thin films with various values of x were deposited on Si（111） substrates by the sol-gel technique. The influence of Mn content on the optical properties was studied by spectroscopic ellipsometry （SE） in the UV–Vis–NIR region. By fitting the measured ellipsometric parameter （Ψ and Δ） with a four-phase model （air/BMT＋voids/BMT/Si（111））, the key optical constants of the thin films have been obtained. It was found that the refractive index n and the extinction coefficient k increase with increasing Mn content due to the increase in the packing density. Furthermore, a strong dependence of the optical band gap Eg on Mn/Ti ratios in the deposited films was observed, and it was inferred that the energy level of conduction bands decreases with increasing Mn content.
文摘Raman and IR spectra of Nb-doped PTC Ba1-xPbxTiO3 semiconducting ceramics (x = 0,0. 28,0. 296,0. 313,0. 330,0. 370) have been measured, and mode assignments of Raman scattering frequencies and infrared absorption peaks have been made at room temperature. The influence of Pb2+ ions content on resistivity temperature characteristics and vibration spectra for the Ea1-xPbxTiO3, ceramics have been discussed,and the temperature dependence of the Raman spectra in tetragonal and cubic phases have been investigated from 25 to 340℃. The results indicated that the Raman spectra of the paraelectric phase above Curie point are obviously different from that of ferroelectric phase below Curie point are obviously different from that of ferroelectric phase below Curie point for all the samples. Curie point of each sample,which is determined by resistivity-temperature characteristic measurment, is in good agreement with the results of Raman analysis. The ferroelectric phase transition in the PTCR Bai-xPbxTiO3 ceramics belongs to a distortion or displacement transition.
基金Project supported by the National Natural Science Foundation of China (Grant Nos. 60871049 and 50972024)
文摘Tunable and switchable Ba 0.5 Sr 0.5 TiO 3 film bulk acoustic resonators（FBARs） based on SiO 2 /Mo Bragg reflectors are explored,which can withstand high temperature for the deposition of Ba x Sr 1 x TiO 3（BST） films at 800 C.The dc bias-dependent resonance may be attributed to the piezoelectricity of the BST film induced by an electrostrictive effect.The series resonant frequency is strongly dc bias-dependent and shifts downwards with dc bias increasing,while the parallel resonant frequency is only weakly dc bias-dependent and slightly shifts upwards at low dc bias（ 45 V） while downwards at higher dc bias.The calculated relative tunability of shifts at series resonance frequency is around 2.3% and the electromechanical coupling coefficient is up to approximately 8.09% at 60-V dc bias,which can be comparable to AlN FBARs.This suggests that a high-quality tunable BST FBAR device can be achieved through the use of molybdenum（Mo） as the high acoustic impedance layer in a Bragg reflector,which not only provides excellent acoustic isolation from the substrate,but also improves the crystallinity of BST films withstanding higher deposition temperature.
基金Project supported by the National Center for Research and Development on Superconducting, the National Natural Science Foundation of China and the National Laboratory of Solid State Microstructure in Nanjing University.
文摘The development of superconductor/insulator/superconductor（SIS）tunnel junctions inthe cuprate high-temperature superconductor family has been hampered by an anisotropicstructure and a coherence length ξ as short as 0.3 nm. However, the discovery of Ba<sub>1-x</sub>K<sub>x</sub>-BiO<sub>3</sub>（x≈0.4） superconductor which is an isotropic cubic structure and has a
