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A complete analysis of magnetization curves is given for bulk sintered samples of Nb3Sn with low hysteresis and for finely powdered sintered and melted samples of Nb3Sn, Nb3Al, V3Si and V3Ga. The Ginzburg-Landau parameterκ and the penetration depthλ of weak magnetic fields is calculated from the temperature dependence of the thermodynamic and upper critical fieldsH c andH c2. The slope of theH c ?T curve is about 360 Oe/°K and approximately the same for all measured samples. There is an extremely high increase of the lower critical fieldH c1 if the grain size approachesλ. The occurence of field expulsion and partially reversible magnetization curves of sintered Nb3Sn samples with high sintering temperatures and high pore volumes is explained by means of connections between single grains which have lower transition temperatures.  相似文献   

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For a typical laser gas discharge, the concentration and temperature of the most important plasma components at the end of the current pulse are calculated on the basis of given data for the tube radius, gas pressure, and energy input. Relating to a postdischarge time up to 1 s, the deionization, the association of the nitrogen atoms, the deexcitation of metastable molecules and the relaxation of the vibration temperature are investigated by means of simple balance equations. Finally the influence of plasma relicts on the following discharge pulse is discussed.  相似文献   

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In an atomic beam magnetic resonance experiment, the hyperfine interaction constantsA andB of the4 I 2/15-groundstate of Ho165 were found to beA=800,58389 (50) MHz,B=?1667,997 (50) MHz. Using an effective value for 〈r ?3〉, the magnetic moment of the Ho165 nucleus was calculated to beμ=4·1(4)μ n . The quadrupolement was determined by use of the 〈r ?3〉 given byWatson andFreeman. The result isQ=2·4·10?24 cm2.  相似文献   

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The presented method is based on an extension of the Goldberger-Adams theorem and on a systematic application of Wick's theorem. The latter leads to combinatorial problems, which in general are complicated but well-fit to be handled by computers. In the two pureJT-casesE-e andT-t the combinatorial problems are simple. In particular in theE-e-case (trigonal) the optical response can be written in a concise analytical form. It is shown further that by means of a one-to-one correspondence of the respective combinatorial problems it suffices to calculate the complete sequence of moments in the strong coupling limit to write down expressions for the optical response with arbitrary coupling, which are exact both in the strong and weak coupling limit.  相似文献   

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