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A thermodynamic model of magnetic insulator-to-metal transitions is presented. As the parameters are varied it shows with increasing temperatures; (a) antiferromagnetic insulator → paramagnetic insulator; or (b) antiferromagnetic insulator → metal → paramagnetic insulator; or (c) antiferromagnetic insulator → metal; or (d) metal at all temperatures. Behaviors (b) and (c) are separated by a classical critical point. The model reproduces well the behavior encounted in (V1-xCrx)2O3 and can be applied to magnetic semiconductors in general. 相似文献
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The pseudopotential form factors used previously by the authors to study the vacancy formation in aluminum are employed to calculate the atom displacements around and formation energy of an interstitial aluminum atom placed at the center (1/2, 1/2, 1/2) of the face-centered cubic unit cell with encouraging results. 相似文献
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Amita Gupta Alexei Yu Ganin Parmanand Sharma Vikrant Agnihotri LM Belova KV Rao Mikhail E Kozlov AA Zakhidov RH Baughman 《Pramana》2002,58(5-6):1051-1059
We present studies of novel nanocomposites of BiNi impregnated into the structure of opals as well as inverse opals. Atomic force microscopy and high resolution elemental analyses show
a highly ordered structure and uniform distribution of the BiNi filler in the matrix. These BiNi-based nanocomposites are
found to exhibit distinct ferromagnetic-like ordering with transition temperature of about 675 K. As far as we know there
exists no report in literature on any BiNi compound which is magnetic. 相似文献
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A simple model for the spin polarization around a charged interstitial impurity in ferromagnetic nickel is presented. It is based on screening of the charge by only s-electrons, while d-electrons, considered to be correlated and localized, are responsible, through an exchange mechanism, for the s-electron spin polarization. Agreement with recent experiments on μ+ precession in Ni, as well as neutron diffraction data is satisfactory. 相似文献
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The behaviour of cyclotron masses for n-type Si(100)/SiO2 inversion layers under stress is explained by means of a charge-density-wave model. The model yields: (1) the observed occupied valley degeneracy of two; (2) a cyclotron mass which varies as a function of stress or as a function of electron number density between 0.19 me and 0.42 me; (3) a charge-density-wave solution only for a restricted range of stresses, with a different paramagnetic solution at each boundary of this range. Of the two tramsitions one is first order and the other second order both as a function of stress and carrier density. The approximations in the calculation are discussed. 相似文献