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991.
Geometric phase of mixed state is expanded for a two-level atom interacting with a quantized field mode, where master equation
is a modified Bloch equation with constant terms that are used to explain emergence of sidebands in the spectrum of the fluorescent
light. The results show that geometric phase transition is observed for medium initial angle when the Rabi frequency associated
with the driving field becomes comparable to the spectral width of the atom. We find that the geometric phase transition depends
on population inversion and Bloch radius, which is helpful to understand mechanism of sideband. 相似文献
992.
T.H. Meen C.J. Huang J.K. Tsai W.R. Chen L.W. Ji 《Journal of Physics and Chemistry of Solids》2011,72(6):653-656
In this research, dye-sensitized solar cells based on TiO2 micro-pillars fabricated by inductive couple plasma etcher were investigated by analyses of X-ray diffraction (XRD), scanning electron microscopy (SEM), contact angle, ultraviolet-visible absorption spectra (UV-vis), and current-voltage characteristics. X-ray diffraction patterns show that the TiO2 anatase phase forms while sintering at 450 °C for 30 min. The SEM images reveal that the diameter and height of TiO2 micro-pillars are about 3 and 0.8 μm, respectively. The measurements of contact angle between TiO2 micro-pillars and deionized water (DI water) reveal that the TiO2 micro-pillars is super-hydrophilic while annealed at 450 °C for 30 min.The absorption spectrum of TiO2 micro-pillars is better than TiO2 thin film and can be widely improved in visible region with N3 dye adsorbed. The results of current-voltage (I-V) characteristics analysis reveal that dye-sensitized solar cell with TiO2 micro-pillars electrode has better I-V characteristics and efficiency than TiO2 film electrodes. This result may be due to the annealed TiO2 micro-pillars applied on the electrode of dye-sensitized solar cell can increase the contact area between TiO2 and dye, resulting in the enhancement of I-V characteristics and efficiency for dye-sensitized solar cell. 相似文献
993.
Ji Sun Im Tae-Sung Bae Young-Seak Lee 《Journal of Physics and Chemistry of Solids》2011,72(10):1175-1179
ZrO2-embedded carbon fibers were prepared for use as an electromagnetic interference (EMI) shielding material by electrospinning and heat treatment methods. Structural changes were observed in the ZrO2 and in the carbon structures by XRD and Raman spectroscopy, respectively. During heat treatment, XRD analysis results revealed a transition from a monoclinic structure to a tetragonal structure in ZrO2 and a graphitization in the structural formation of carbon fibers was observed by Raman spectroscopy. It was observed that these structural changes in the ZrO2 and the carbon fibers improved the real and imaginary permittivities by a factor of more than 3.5. The EMI shielding efficiency (SE) improved along with the permittivity with higher treatment temperatures and greater amounts of embedded ZrO2; the highest average EMI SE achieved was 31.79 dB in 800-8500 MHz. The heat treatment played an important role in the improvements in the permittivity and in the EMI SE because of the heat-induced structural changes of the ZrO2-embedded electrospun carbon fibers. We suggest that the EMI shielding of the fibers is primarily due to the absorption of electromagnetic waves, which prevents secondary EMI by reflection of electromagnetic waves. 相似文献
994.
S.J. Young C.H. Hsiao L.W. Ji T.P. Chen K.J. Chen 《Journal of Physics and Chemistry of Solids》2011,72(2):147-149
The authors report the fabrication of ZnO-based metal-oxide-semiconductor field effect transistors (MOSFETs) with a high quality SiO2 gate dielectric by photochemical vapor deposition (photo-CVD) on a sapphire substrate. Compared with ZnO-based metal-semiconductor FETs (MESFETs), it was found that the gate leakage current was decreased to more than two orders of magnitude by inserting the photo-CVD SiO2 gate dielectric between ZnO and gate metal. Besides, it was also found that the fabricated ZnO MOSFETs can achieve normal operation of FET, even operated at 150 °C. This could be attributed to the high quality of photo-CVD SiO2 layer. With a 2 μm gate length, the saturated Ids and maximum transconductance (Gm) were 61.1 mA/mm and 10.2 mS/mm for ZnO-based MOSFETs measured at room temperature, while 45.7 mA/mm and 7.67 mS/mm for that measured at 150 °C, respectively. 相似文献
995.
Jo JY Chen P Sichel RJ Callori SJ Sinsheimer J Dufresne EM Dawber M Evans PG 《Physical review letters》2011,107(5):055501
The nanosecond response of a PbTiO(3)/SrTiO(3) ferroelectric/dielectric superlattice to applied electric fields is closely linked to the dynamics of striped domains of the remnant polarization. The intensity of domain satellite reflections observed with time-resolved x-ray microdiffraction decays in 5-100 ns depending on the magnitude of the electric field. The piezoelectric response of the superlattice within stripe domains is strongly suppressed due to electromechanical clamping between adjacent regions of opposite polarization. Regions of the superlattice that have been switched into a uniform polarization state by the applied electric field, however, exhibit piezoelectricity during the course of the switching process. We propose a switching model different from previous models of the switching of superlattices, based instead on a spatially heterogeneous transformation between striped and uniform polarization states. 相似文献
996.
We investigate numerically the effects of higher-order space-charge field on the self-deflection of bright photovoltaic spatial solitons in two-photon photovoltaic photorefractive crystals under steady-state conditions. The expression for an induced space-charge electric field, including higher-order space-charge field terms is obtained. The dynamical evolution equation is built in which the effects that arise from these higher-order terms are considered. Numerical results indicate that bright photovoltaic solitons can bend towards both the same direction as the crystal's c-axis and the opposite direction, respectively. Specifically, self-deflection cannot occur for bright photovoltaic solitons if the strength of the photovoltaic field and the intensity of the input beam are appropriately selected. Relevant examples are provided. 相似文献
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