Windows 9.x下的设备驱动程序

本文首先介绍了Windows 9.x下的驱动程序，并阐述了虚拟机、保护模式的概念，然后对VxD的原理进行了说明。最后，介绍了两种开发VxD的工具。     

Windows 9.x下的设备驱动程序

本文首先介绍了Windows9.x下的驱动程序 ,并阐述了虚拟机、保护模式的概念 ,然后对VxD的原理进行了说明。最后 ,介绍了两种开发VxD的工具。     

Superconducting and normal state properties of Li1+x Ti2−x O4 spinel compounds. II. Low-temperature heat capacity

Heat capacity data are reported which confirm as a bulk effect the previously reported superconductivity in LiTi ₂ O ₄ . These data also establish LiTi₂O₄ as a weak couplingd-band superconductor with superconducting state properties well described by the Bardeen—Cooper—Schrieffer theory of superconductivity. The properties of LiTi ₂ O ₄ are compared with those of other superconducting spinel compounds, and the composition dependence ofT _c for Li _1+x Ti _2–x O ₄ is discussed. The disappearance of superconductivity forx0.1 was found to be correlated with a rapid decrease in the normal-state linear heat capacity coefficient.Research sponsored by the U.S. Energy Research and Development Administration under Contract No. ERDA E(04-3)-34 PA227.Research sponsored by the Air Force Office of Scientific Research, Air Force Systems Command, USAF, under AFOSR Contract Number AFOSR/F-44620-72-C-0017.     

Deposition of SixC1−x:H films by reactive r.f. sputtering

The preparation of thin Si_xC_{1 − x}:H films at low temperatures by reactive r.f. sputtering in acetylene-argon gas using pure silicon wafers as target material was investigated. Optimum conditions for SiC deposition were selected by variation of r.f. power density, r.f. peak voltage and the acetylene partial pressure. The deposited Si_xC_{1 − x}:H films were characterized by density measurements, transmission high energy electron diffraction, transmission electron microscopy and UV and IR transmission spectroscopy as well as by electron probe microanalysis and X-ray photoelectron spectroscopy analysis. It is seen that the chemical composition and the structure of reactively sputtered Si_xC_{1 − x}:H films are strongly influenced by the ratio of the acetylene content in the plasma to the power density used. For acetylene contents smaller than 7.5 vol.% in the glow discharge, polycrystalline β-SiC films can be prepared if the r.f. power density is limited to 4.6 W cm⁻².     

Electrical properties of N.T.C. thermistors made of manganite ceramics of general spinel structure: Mn3 − x − x′MxNx′O4 (0 ≤ x + x′ ≤ 1; M and N being Ni, Co or Cu). Aging phenomenon study

In this paper, we report our results on the electrical properties and aging phenomenon (or resistance drifts) of Negative Temperature Coefficient thermistors manufactured out of manganite ceramics of general spinel structure: Mn_{3 – x – x}M _x N _xO₄ (0 x + x 1; M and N being Ni, Co or Cu). It is shown that the resistance drift is not a result of the use of metallic electrodes or metal/ceramic interfaces. However, thermal treatment used to bond metallic electrodes on ceramics triggers the electrical aging. Components with almost no electrical drift can be obtained by carefully controlling this metallization treatment. Beyond this experimental result we have tried to determine a suitable basic origin explaining the aging of NTC. Depending on the studied solid solutions, i.e. cations involved in the spinel structure, many overlapping complex ionic diffusion mechanisms might be operating. However, our study suggests that electrical aging might be triggered by the high mobility of Mn³⁺ cations which have the tendency to gather in clusters in such oxide structure.     

Specific heat capacity of molybdenum chalcogenides. III. Measurements of the heat capacity of Sn1 − x Ga x Mo5S6. An investigation of the singularities at low temperatures

The heat capacity of molybdenum chalcogenides with different Sn/Ga content was measured at temperatures of T 60 K. The occurrence of two phases of the chalcogenides studied could clearly be seen for higher Ga concentrations. In the miscibility gap there coexists a superconducting phase (T _c= 12.5 K) SnGa_0.25Mo₅S₆ with the ferromagnetic GaMo₅S₆ phase (T _curie = 19 K). As for the pure ternary compound GaMo₅S₆, a singularity of the heat capacity could also be observed in the range of the structural change (T = 45 K). All the singularities are discussed.     

Pb1−x Bi x /Bi/Pb1−x Bi x Josephson junction

A superconductor/semimetal/superconductor (S/SM/S) Josephson junction has been developed. We have used an alloy of Pb_1–x Bi _x (0x 0.6) as the superconductor and Bi as the semimetal. By irradiating at X-band microwave of 10 GHz, Shapiro steps were observed for various bismuth barrier thicknesses inÅ and bismuth weight ratiosx. Finally, we obtained the empirical relationship for barrier thickness, below which microwaves could be detected for various bismuth weight ratiosx at the temperature of 4.2 K.     

Lattice-matched epitaxial Pb1 − x Mn x Se/PbSe1 − x S x heterojunctions

This paper examines the possibility of producing lattice-matched p-n heterojunctions based on epitaxial n-Pb_{1 ? x} Mn _x Se (x = 0.02) and p-PbSe_{1 ? x} S _x (x = 0.04) films. The heterojunctions have been grown by molecular beam epitaxy in a single processing cycle, without breaking the vacuum, using a compensating Se vapor source in the growth process. Optimal conditions have been found for the growth of structurally perfect (W _1/2 = 90″-100″) epitaxial films and fabrication of lattice-matched heterojunctions based on such films, photosensitive in the IR spectral region.     

Thermodynamic properties of Ca1 − x Er x F2 + x and Ca1 − x Yb x F2 + x heterovalent solid solutions

The heat capacity of single crystals of the Ca_{1 ? x} Er _x F_{2 + x} (x = 0.05, 0.10) and Ca_0.95Yb_0.05F_2.05 fluorite solid solutions was determined by adiabatic calorimetry in the temperature range 55–300 K. The results were used to obtain temperature dependences of the Debye characteristic temperature, entropy, and enthalpy for the solid solutions.     

High-Pressure Studies on Superconductivity in LaFeAsO1−x F x and SmFeAsO1−x F x

The pressure dependence on the superconducting transition temperature (T _c ) was investigated for the iron-based superconductors LaFeAsO_1−x F _x and SmFeAsO_1−x F _x . The T _c ’s increase largely for LaFeAsO_1−x F _x with a small increase of pressure, while a sharp decrease of T _c was observed for SmFeAsO_1−x F _x . The electrical resistivity measurements reveal pressure-induced superconductivity for undoped LaFeAsO and SmFeAsO. These pressure effects seem to be related to an anisotropic decrease of the lattice constants under high pressure from the x-ray diffraction measurements up to 10 GPa for the LaFeAsO_1−x F _x system.     

The dielectic response of K x Al x Ti8−x O16 and K x Mg x/2 Ti8−x/2 O16

Materials of the hollandite structure with the general formulae K_x Al_x Ti_8–x O₁₆ and K_x Mg_x/2 Ti_8–x/2 O₁₆ have been synthesized in the composition range 1.6x2.0 and their dielectric properties have been measured in the temperature range 77 to 800 K and the frequency range 10^–3 to 10⁶ Hz. The observed response shows a whole range of features characteristic for both charge carrier and dipolar polarization processes and these are seen as being associated with the one-dimensional transport in channels in the hollandite structure. At low temperatures the dominant response is the universal dielectric relation in which the loss follows the law x() ^n–1, with the exponent n<1 and equal specifically to approximately 0.7. This is followed at 120 to 180 K by a distinct loss peak superimposed on the above law, and finally at higher temperatures by a region of strong dispersion which is associated with strongly interacting many-body processes between charged carriers restricted by defects to move in limited regions of the channels.     

Dielectric properties of the Sr1−x La x Sn1−x Co x O3 system

The possibility of the formation of a solid solution in the Sr_1–x La _x Sn_1–x Co _x O₃ system has been explored. Single-phase solid solution forms in the compositions for x0.10. All single-phase solid solution compositions have a cubic structure similar to SrSnO₃. The dielectric behaviour of these solid solution compositions has been studied as a function of temperature and frequency. The frequency dependence of dielectric constant and dielectric loss in these materials indicates that space charge polarization contributes significantly to their observed dielectric parameters. Microstructural studies show the presence of well-faceted grains. The average grain size in these samples is small.     

New plasma deposition process of amorphous GaxAs1−x in an r.f. capacitively coupled diode system

A new process to obtain hydrogenated a-Ga_xAs_1−x (amorphous alloys) by glow discharge in an r.f. capacitively coupled system is described. These alloys are obtained from metallic gallium and arsine gas (AsH₃). A novel use of simultaneous sputtering and gas decomposition in the same system allows the control of the deposition. The composition of a-Ga_xAs_1−x is monitored by the gas phase composition. The conduction mechanisms are shown to be strongly dependent on gallium or arsenic in excess.     

Fabrication and microstructure of the d.c.-magnetron-sputtered YBa2Cu3O7 − x superconducting thin films

Systematic investigations were conducted to determine the effect of deposition conditions on the microstructure and superconducting properties of YBa₂Cu₃O_{7 – x} thin films produced by d.c. magnetron sputtering on (001) MgO substrate. The films were c-axis preferentially oriented with respect to the (001) MgO surface at substrate temperatures of 680–700 C. X-ray diffraction patterns clearly indicated the existence of the c-axis alignment normal to the substrate surface and some second phases. The second phases, including a Cu-rich phase and Y₂O₃, were identified by energy dispersive X-ray spectrometer and the microstructures were analysed by electron and atomic force microscopes.     

Crystallization behaviour of amorphous Sc100−x Fe x alloys near x=25 composition

A detailed study of the process of crystallization in amorphous Fe₂₅Sc₇₅, Fe₂₈ Sc₇₂ and Fe₂₅Sc₄₅Zr₃₀ alloys has been carried out using differential scanning calorimetry, X-ray diffraction and Mössbauer spectroscopic techniques. The complex multi-stage transformation process in Fe₂₅Sc₇₅ and Fe₂₈Sc₇₂ is understood in terms of polymorphous formation of an intermediate metastable crystalline phase of orthorhombic structure (a = 0.521 nm, b = 0.648 nm and c = 1.212 nm) and of likely Sc₃Fe stoichiometry, before final eutectic crystallization to stable Fe₂Sc and -Sc.     

Synthesis of Cr x Ti1−2x Nb x O2O20≤x≤0.5 rutile solid solutions from alkoxides

In this study, Cr _x Ti_1–2x Nb _x O₂ (0 x 0.5) rutile solid solutions have been synthesized from gels built from hydrolysis-condensation of Cr (III) acetylacetonate, NbCl₅ and Ti (IV) isopropoxide mixture (polymeric gel). Characterization of these solid solutions was carried out by X-ray diffraction, ultraviolet-visible and infrared spectroscopy, differential thermal and thermogravimetric analysis and CIELAB (Commission Internationale del'Eclairage L^*a^*b^*) parameter measurements. The results obtained by the polymeric gel method were compared with those obtained by traditional ceramic synthesis. This comparison reveals some differences with regard to synthesis temperatures and reaction mechanisms. The formation of Cr _x Ti_1–2x Nb _x O₂ (0 x 0.5) rutile solid solutions by the ceramic method requires temperatures of about 1200°C and soaking times of several days. These solid solutions are synthesized at 1000°C in 24 h by the polymeric gel method. In ceramic synthesis, the CrNbO₄ compound with rutile structure appears as an intermediate compound in the formation of rutile solid solutions. In polymeric gel synthesis, however, the CrNbO₄ rutile compound was not detected in the samples.     

Bond Angle Study of Self-compensating Y1−x Ca x Ba2−x La x Cu3O z System

Single-phase samples of a self-compensating Y_1?x Ca _x Ba_2?x La _x Cu₃O _z system were synthesized through a solid-state reaction method with x<0.4. The structure of all samples were characterized by X-ray diffraction and refined by the Rietveld method. Superconducting properties have been investigated by the DC magnetization measurement. The critical temperature (T _c ) decreases evidently with the increment of x although the carrier concentration remains constant in the samples for different doping level. Careful study of the chemical bonds in the crystalline lattice demonstrates that the T _c is closely correlated to four pairs of bond angles in the unit cell. The analysis indicates that crystalline structure is one of the important factors to high-T _c superconductivity, and its influence is independent of the carrier concentration.     

Crystallization kinetics of Zr-rich FexZr0−x0−x0−x(20 ⩽ x ⩽ 40) metallic glasses

The crystallization kinetics of the melt-spun Fe-Zr metallic glasses in the iron-rich region has been investigated by means of DSC and X-ray diffraction. The crystallization mode changes with iron concentration. In the lower iron region, 20 x 25, the Fe _x Zr100–x glasses crystallize into -Zr and Ti₂Ni-type FeZr₂ with an accompanying sharp and large exotherm at the first crystallization step and immediately after this step, they transform into orthorhombic FeZr₃. On the other hand, the alloys with 35 x 40 exhibit a gradual exotherm which initiates from a temperature far below the definite crystallization temperature (T _x). The Fe-Zr metallic glasses in this concentration region crystallize polymorphously into the oxygenstabilized Ti₂Ni-type FeZr₂ with accompanying relatively small and composite exotherms. The annealing at a temperature where the gradual exotherm occurs for the alloys with 30 x 40 does not cause any changes of X-ray halo pattern but results in the reduction of the heat of exotherm due to the crystallization.     

Homogeneous Coexistence in CaFe1−x Co x AsF and Phase Segregation in LaFeAsO1−x F x Studied via NMR

In iron-based pnictides, one of the interesting topics is homogeneous coexistence or phase segregation at the boundary between antiferromagnetic (AF) and superconducting (SC) phases. We addressed this problem on a microscopic level by means of ⁷⁵As NMR measurements in LaFeAsO_1?x F _x (x=0.026) (La1111), and CaFe_1?x Co _x AsF (x=0.06) (Ca1111) having an intermediate electronic phase diagram between Ba(Fe_1?x Co _x )₂As₂ and the La1111 series. NMR spectra for 6 % Co-doped Ca1111 samples were very similar to those for the undoped samples even below T _c , suggesting homogeneous coexistence of the AF and SC states. For 2.6 % F-doped La1111 samples, AF and paramagnetic (PM) domains coexist at ambient pressure, and AF and SC domains coexist at 3.0 GPa. The coexistence of domains is explained by considering a SC dome separated from the AF phase in the phase diagram. The homogeneous coexistence support S _±-wave superconductivity, whereas separation of the AF and SC phases gives credence to S ₊₊-wave superconductivity.