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Closing of a spin gap and ferromagnetism induced by magnetic impurities: finite-size effects and critical exponents

机译:磁性杂质引起的自旋间隙和铁磁性的闭合:有限尺寸效应和临界指数

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We consider the one-dimensional gas of electrons interacting via an attractive delta -function potential. The attractive potential leads to the formation of Cooper-pair-like bound states with a spin gap. Without destroying the integrability, we introduce a finite concentration of mixed-valence impurities with two magnetic configurations of spin S and S + 1/2, which hybridize with the conduction states of the host. We derive the Bethe ansatz equations diagonalizing the system for the correlated host with impurities and discuss the ground-state properties as functions of the concentration of impurities and the Kondo coupling. For a sufficiently large density of electrons the spin gap is reduced by the impurities and is closed at a critical concentration which depends on the impurity spin and the coupling strength. A ferromagnetic phase of unpaired spin-polarized itinerant electrons is induced for impurity concentrations larger than the critical one. The critical behaviour of the correlation functions is studied in the gapped and gapless regions using the mesoscopic energy spectrum and conformal field theory. [References: 49]
机译:我们认为电子的一维气体通过有吸引力的三角函数势相互作用。诱人的电势导致形成具有自旋间隙的库珀对状结合态。在不破坏可积性的情况下,我们引入了有限浓度的混合价杂质,它们具有自旋S和S + 1/2的两种磁性构型,它们与主体的导电态混合。我们推导了Bethe ansatz方程,该方程对角化了带有杂质的相关主体的系统,并讨论了基态特性与杂质浓度和Kondo耦合的关系。对于足够大的电子密度,自旋间隙会被杂质减少,并以取决于杂质自旋和耦合强度的临界浓度封闭。当杂质浓度大于临界浓度时,会感应出不成对的自旋极化巡回电子的铁磁相。利用介观能谱和共形场理论研究了间隙和无间隙区域中相关函数的临界行为。 [参考:49]

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