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111.
Zinc blende (ZB) CdSe hollow nanospheres were solvothermally synthesized from the reaction of Cd(NO3)2·4H2O with a homogeneously secondary Se source, which was first prepared by dissolving Se powder in the mixture of ethanol and oleic acid at 205 °C. As Se power directly reacted with Cd(NO3)2·4H2O in the above mixed solvents, wurtzite (W) CdSe solid nanoparticles were produced. Time-dependent experiments suggested that the formation of CdSe hollow nanospheres was attributed to an inside-out Ostwald ripening process. The influences of reaction time, temperature and ethanol/oleic acid volume ratio on the morphology, phase and size of the hollow nanospheres were also studied. Infrared (IR) spectroscopy investigations revealed that oleic acid with long alkene chains behaved as a reducing agent to reduce Se powder to Se2− in the synthesis. Photoluminescence (PL) measurements showed that the ZB CdSe hollow nanospheres presented an obvious blue-shifted emission by 42 nm, and the W CdSe solid nanoparticles exhibited a band gap emission of bulk counterpart. 相似文献
112.
Cristian E. Botez David Carbajal Ronald J. Tackett 《Journal of Physics and Chemistry of Solids》2010,71(11):1576-1580
We have used synchrotron X-ray diffraction to investigate the structural and chemical changes undergone by polycrystalline KH2PO4 (KDP) upon heating within the 30-250 °C temperature interval. Our data show evidence of a polymorphic transition at T∼190 °C from the room-temperature tetragonal KDP phase to a new intermediate-temperature monoclinic KDP modification (spacegroup P21/m and lattice parameters a=7.590, b=6.209, c=4.530 Å, and β=107.36°). The monoclinic RDP polymorph remains stable upon further heating to 235 °C, and is isomorphic to its RbH2PO4 and CsH2PO4 counterparts. 相似文献
113.
114.
Frequency domain (FD) fluorescence lifetime data was collected for a series of 20 crude petroleum oils using a 405 nm excitation
source and over a spectral range of ~426 to ~650 nm. Average fluorescence lifetimes were calculated using three different
models: discrete multi-exponential, Gaussian distribution, and Lorentzian distribution. Fitting the data to extract accurate
average lifetimes using the various models proved easier and less time consuming for the FD data than with Time Correlated
Single Photon Counting (TCSPC) methods however the analysis of confidence intervals to the computed average lifetimes proved
cumbersome for both methods. The uncertainty in the average lifetime was generally larger for the discrete lifetime multi-exponential
model when compared to the distribution-based models. For the lifetime distributions, the data from the light crude oils with
long lifetimes generally fit to a single decay term. Heavier oils with shorter lifetimes required multiple decay terms. The
actual value for the average lifetime is more dependant on the specific fitting model employed than the data acquisition method
used. Correlations between average fluorescence lifetimes and physical and chemical parameters of the crude oils were made
with a view to developing a quantitative model for predicting the gross chemical composition of crude oils. It was found that
there was no significant benefit gained by using FD over TCSPC other than more rapid data analysis in the FD case. For the
FD data the Gaussian distribution model for fluorescence lifetime gave the best correlations with chemical composition allowing
a qualitative correlation to some bulk oil parameters.
相似文献
Alan G. RyderEmail: |
115.
K. Morawetz C. Olbrich S. Gemming 《The European Physical Journal B - Condensed Matter and Complex Systems》2008,62(3):311-317
The coverage of vicinal, stepped surfaces with molecules is simulated with
the help of a two-dimensional Ising model including local distortions and
an Ehrlich-Schwoebel barrier term at the steps. An effective two-spin model is capable
to describe the main properties of this distorted Ising model. It is employed
to analyze the behavior of the system close to the critical points.
Within a well-defined regime of bonding strengths and Ehrlich-Schwoebel barriers we
find a reduction of coverage (magnetization) at low temperatures due to the
presence of the surface step. This results in a second, low-temperature
transition besides the standard Ising order-disorder transition.
The additional transition is characterized by a divergence of the
susceptibility as a finite-size effect. Due to the
surface step the mean-field specific heat diverges with a power law. 相似文献
116.
We had already obtained the analytical solutions for the compression wave and steady-state oscillating flow in a pipe with a circular cross section [Sato Y, Kanki H. Formulas for compression wave and oscillating flow in circular pipe. To be published in Appl Acoust [accepted 11 Sept. 2006]]. This work contains three key-components. The first key is to simplify the formulas using the unique mathematic technique without losing the accuracy. Simplifying the formulas is the one of the most important factors for formulas used in engineering use. The results will enable us to greatly reduce the work and computation costs. The second is to verify the flow distribution calculated by our formulas. The third is to study the possibility of application of our method to the analysis in turbulent flow region. Kawata et al. have represented the validity of one-dimensional quasi-analysis in turbulent flow region, using the method of D’Souza et al. and the shear viscosity. Therefore, in this paper the validity of the analysis in a turbulence region was verified by proving theoretically that the methods of D’Souza et al. and ours are intrinsically equivalent. The proof of equivalence was accomplished using the formulas simplified in this paper. 相似文献
117.
M. Marqués 《Journal of Physics and Chemistry of Solids》2008,69(9):2277-2280
We report first principles results of a detailed investigation directed to elucidate mechanistic aspects of the zircon-reidite phase transition in ZrSiO4. The calculated thermodynamic boundary is located around 5 GPa, and the corresponding thermal barrier, estimated from temperatures at which the transition is observed at zero and high pressure, is 133 kJ/mol. Under a martensitic perspective, we examine two different transition pathways at the thermodynamic transition pressure. First, the direct, displacive-like, tetragonal I41/a energetic profile is computed using the c/a ratio as the transformation parameter, and yields a very high activation barrier (236 kJ/mol). Second, a quasi-monoclinic unit cell allows us to characterize a transition path from zircon (β=90°) to reidite (β=114.51°) with an activation barrier of around 80 kJ/mol at β=104°. This energy is somewhat lower than our previous estimation and supports the reconstructive nature of the transformation at the thermodynamic transition pressure. 相似文献
118.
T. Takano 《Journal of Physics and Chemistry of Solids》2008,69(12):3089-3092
We investigated band-insulator-to-superconductor transition in LixZrNCl driven by carrier doping by means of magnetization, resistivity, and optical reflectivity measurements. The magnetization and the resistivity measurements showed that the transition occurs at around x=0.05. The pristine β-ZrNCl exhibited reflectivity and optical conductivity spectra typical of an insulator, whereas in the spectrum of Li0.37ZrNCl, Drude-like high reflectance band and associated plasma edge are apparently observed. This is the direct spectroscopic evidence of insulator-to-metal transition of LixZrNCl. 相似文献
119.
120.
Nadine Werth Mathias S. Müller Johann Meier Alexander W. Koch 《Optics Communications》2011,284(9):2317-2322
Using Laser-based Speckle-Interferometers, the shape of optically rough surfaces can be measured precisely and contactlessly from variable measuring distances even in regions of difficult access. This work is concerned with the integration of a micromirror array (MMA) into an electronic Speckle-Pattern-Interferometer. With the adaptive optics, it is intended to adapt the phasefront of a reference wave to critical surface areas of the measurement object. Yet, due to the topography of the MMA, diffraction effects occur which affect the phase and intensity of the generated wavefront. We demonstrate how these diffraction effects can be efficiently modelled by a Fraunhofer diffraction method. We compare the results of this model to theoretical data obtained by a numerical Fresnel diffraction model and to measurement data obtained from a measurement setup incorporating a multi mirror array. 相似文献