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1.
The morphology of the silver films deposited and annealed on laser ablated YBa2Cu3O7– thin films and the corresponding contact resistivity have been systematically investigated. A minimum contact resistivity of 6 × 10–8 cm2 was reached at 77 K by annealing Ag/YBa2Cu3O7– contact at the optimum temperature. The effect of the annealing temperature on the contact resistivity was explained by considering the morphology of the silver films and the diffusion of silver into YBa2Cu3O7– film, etc. The difference of the contact resistivity for Ag contact to polycrystalline, single crystal and thin film of YBa2Cu3O7– were also explained.  相似文献   

2.
The effect of intraatomic absorption of the L1 X-ray emission line of uranium was studied. To eliminate the effect of the L I I I absorption edge on the chemical shift () of the L1 line, the dependence of L1 on the oxygen index x in oxide systems of variable composition UO2 + x was determined indirectly. It was shown that, in the absence of the effect of the L I I I absorption edge, the dependence of L1 on x is ordinary and, as in the case of other hard emission lines of the uranium L series, can be described by a second-order polynomial. The abnormal dependence of L1 on x is explained.  相似文献   

3.
Conclusions It is possible by means of the above resonator, according to our analysis and in the absence of air gaps between the sample and the line, to evaluate the real components and of permeability and permittivity respectively in the range of 2 to 100 with an error between ±3% and ±10% in the temperature range from room temperature to +400°C, and the imaginary components and (for tan and tan in the range of 0.001 to 2) with an error of 7 to 20% over the same temperature range.  相似文献   

4.
Summary This paper considers a random walk type Markov decision process in which the state spaceI is an integer subset of IR m , and the action spaceK is independent ofi I. The natural order, overI, and a quasi order,, overK, is assumed, together with aconditional convexity assumption on the returns {r i k }, and certain other assumptions about these rewards and the transition probabilities in relationship to the orders and.A negatively isotone policy is one for whichi i(i))(i) (i.e.(i) (i) or(i) i)). It is shown that, under specified conditions, a negatively isotone optimal policy exists. Some consideration is given to computational implications in particular relationship to Howard's policy space method.
Zusammenfassung Wir betrachten einen Markovschen Entscheidungsprozeß vom random walk Typ. Der ZustandsraumI sei eine Teilmenge des IRm, wobeii I ganzzahlige Komponenten habe. Die MengeK der zulässigen Aktionen ini I sei unabhängig voni I. Sei die natürliche Ordnung aufI und sei eine Quasiordnung aufK. Die Erträge {r i k }seienbedingt konvex, darüberhinaus seien weitere Voraussetzungen über diese Erträge und die Übergangswahrscheinlichkeiten in Bezug auf die Ordnungen und erfüllt. Eine Politik heißt negativ isoton, falls ausi i folgti(i) (d. h.(i) (i) oder(i)(i)). Wir zeigen, daß unter gewissen Voraussetzungen einenegativ isotone optimale Politik existiert: Auch diskutieren wir einige Folgerungen für die Numerik, insbesondere hinsichtlich Howards Politikiteration.
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5.
The causes of a discrepancy in the results of measurements of He II viscosity below T 1.6 k obtained with different measurement methods are investigated. It is shown that to obtain correct results in oscillation experiments, the condition ph should obtain, where is the depth of viscous wave penetration and ph is the phonon free path length. Results of viscosity measurements at different ratios /ph (by a wire viscometer) are presented. It is shown that for the condition ph, the results obtained are in good agreement with the results of Andronikashvili (in which /ph > 100). If the mentioned relation is not satisfied, then, as the value of the ratio /ph is decreased, the value measured for the viscosity is increasingly lower than the results of Andronikashvili.  相似文献   

6.
The superplasticm- curves of Ti-6Al-4 alloy have been determined at different temperatures and strain rates; all were of them L=m max type, and were of either fundamental, descending or ascending types. The latter two types were transformed from the former through the processes ofm Lm O, LO andm Lm F, LF, respectively. The highest total elongation, F, was 1150% obtained at 950C and 1.55×10–3 s–1. The Chin Liu equation has been applied to all types ofm- curves. The parameters characteristic of all types ofm- curves have been obtained and were found to vary with temperature and strain rate. The total elongation, F, is determined by the resultant effects of all other parameters, not by a singlem value, theoretically considered to be constant and determined practically by a tensile strain of about 30%–50% (m 30%–50%) as usual.Nomenclature C (=k/k o ) the normalized slope ofm- curve corresponding to - a material constant corresponding to - m strain-rate sensitivity index corresponding to - m max maximum on them- curve corresponding to L - m min minimum on them- curve corresponding to L - crosshead speed during the tensile test - the strain of the entire stretching process (has same significance as ordinarily adopted ) - F total elongation at fracture chosen for the present work - I intermediate strains including I1, I2, I3, ..., I(i–1), Ii , I(i+1), ..., chosen for the present work - L limit strain separatingm- curves into sections - O (=0) starting strain - strain rate - flow stress  相似文献   

7.
Minor quantities of Ag have been added to Al–Li–Cu–Mg–Zr alloys. Their microstructure has been studied by means of optical metallography, transmission electron microscopy and X-ray diffraction. In the high Li, low Cu : Mg ratio alloys the main phases found were , , S and T1, while fewer T2 and Al7Cu2Fe precipitates were also observed. The addition of up to 0.5 wt% Ag diminishes the and T1 precipitates size. This is attributed to a small increase of Li solubility in the matrix. In the low Li, high Cu : Mg ratio alloy the addition of 0.2 wt % Ag resulted in the precipitation of phase simultaneously with , , S and T1 phases. Due to the low Li concentration an unusual growth of the / precipitates at the expense of the precipitates was also observed.  相似文献   

8.
We present data on the copper isotope effect (63Cu-65Cu), Cu =-nTc/nmCu, for two isotopic pairs of oxygen-deficient YBa2Cu3O7–, where varies between 0.06 and 0.52. Cu is below 0.01 at =0.06 (fully oxygenated), it takes values between –0.14 and –0.34 in the 60 K plateau. Larger negative values of Cu are observed away from the plateau. The dependence of Cu is similar to that of the pressure effect dnTc/dP.  相似文献   

9.
A mathematical model for studying the propagation of long internal ocean waves of finite amplitude is proposed. The vertical structure of the pressure perturbation is investigated and reduced to a Sturm–Liouville eigenvalue problem. In the continuous stratification case, the pattern of this vertical structure depends on the choice of the characteristic scale of a varying stratification parameter, denoted by . As this parameter asymptotically approaches a critical value (i.e. cri), the amplitudes of the solution's normal modes increase considerably. The internal waves break and produce an unstable interface, which degenerates into a turbulent mixed layer. These conditions correspond to the critical state of wave existence. When < cri a three-layer discontinuous gradient model is proposed to resolve the problem. It consists in specifying one solution within a thin intermediary layer and two solutions on either side of this layer. The results show that the use of appropriately matching interfacial conditions allows to obtain generally matching solutions, even for small values of the nonconstant stratification parameter .  相似文献   

10.
Energy losses to radiation of internal waves during the vertical motion of a point dipole in two-dimensional and three-dimensional cases are computed.Notation o(z), po(z) density and pressure of the ground state - z vertical coordinate - v, p, perturbed velocity, pressure, and density - H(d 1n o/dz)–1 characteristic length scale for stratification - N=(gH–1–g2c o –2 )1/2 Weisel-Brent frequency - g acceleration of gravity - co speed of sound - vertical component of the perturbed velocity - V vector operator - k wave vector - frequency - d vector surface element - W magnitude of the energy losses - (t), (r) (x)(y)(z) Dirac functions - vo velocity of motion of the source of perturbations - d dipole moment of the doublet - o,l length dimension parameters - o intensity of the source Translated from Inzhenerno-Fizicheskii Zhurnal, Vol. 39, No. 4, pp. 619–623, October, 1980.  相似文献   

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