掺杂Kondo绝缘体的理论研究

掺杂Ｋｏｎｄｏ绝缘体的理论研究李正中（南京大学物理系，南京，２１０００８）关键词Ｋｏｎｄｏ空穴；Ｋｏｎｄｏ绝缘体；重费米子金属Ｋｏｎｄｏ绝缘体（ＫＩ）是４ｆ族化合物中新发现的一类绝缘性基态重费米子（ＨＦ）材料，包括Ｃｅ３Ｂｉ４Ｐｔ３，ＣｅＮｉＳｎ和Ｃ...

平行双量点中的Fano-Kondo

通过么正变换得到了平行双量子点有间库仑作用时的Fano-Anderson哈密顿量,并用格林函数运动方程的方法济南市出了与实验观测量密切相关的推迟和量子分布格林函数。借助于新得到的哈密顿量和格林函数,可以研究Kondo和Fano共振的关联效应。

嵌入三端传输量子点的介观环的可调Kondo效应

我们借助Anderson模型、利用格林函数方法从理论上研究了一个嵌入三端传输量子点的介观环的Kondo效应。我们发现这个系统的Kondo效应敏感地依赖于系统的宇称，我们调节粒子源与量子点之间地耦合强度可以达到调节Kondo屏蔽云地目的。这为我们测定Kondo屏蔽云的大小和纳米器件的制作提供了一个性能良好的模型。

磁性杂质对量子点内电子态密度Kondo峰的影响

讨论了一个耦合于量子点的磁性杂质,当两边是铁磁性导线时量子点上电子的态密度Kondo峰的变化情况。用格林函数运动方程的方法和特定的自洽方法得到了态密度的解析表达式。杂质与量子点上电子的耦合使得原本简并的电子能级分裂。数值计算结果表明当两边的铁磁导线极化反平行时,态密度的Kondo峰几乎不随着磁性杂质方位角的变化而变化。当极化平行时,会出现3个Kondo峰,并且峰之间的间隔随着杂质的方位角的增大而增大。如果选取适当极化率的铁磁导线,由导线的铁磁性引起的Kondo峰的分裂可以被杂质的耦合作用抵消掉。

Kondo型重费密子超导系统的磁化率和能隙

在P波机制下采用周期Anderson模型Hamilton量,运用Green函数方法讨论Kondo型重费密子超导系统的磁化率和能隙随温度的变化.

基于Ono-Kondo格子模型的超临界页岩气吸附试验研究

页岩储层普遍埋藏较深,地层温度和压力较高,相当一部分页岩气在储层中处于超临界吸附状态。超临界吸附与传统亚临界吸附在机理上有着较大区别,将建立在亚临界条件的吸附模型运用到超临界页岩气吸附领域仍然面临一些挑战。因此,准确表征超临界页岩气吸附是精准评估页岩气储量和制定合理开发方案先决条件。针对页岩中超临界甲烷吸附问题,借助高精度磁悬浮天平重量法吸附仪,开展了高温高压甲烷吸附实验,分别测定了超临界甲烷在40,60,80和100℃的气体相密度和等温吸附曲线。实验结果表明:磁悬浮天平能同时测定气体相甲烷密度和过剩吸附量;超临界甲烷过剩吸附量随压力先增加后减小,过剩吸附量随温度升高而降低,最大过剩吸附量对应的压力随温度升高而升高。在不对吸附相密度和体积做任何假设的前提下,利用Ono-Kondo格子模型分别分析了页岩气的单层和多层吸附。Ono-Kondo格子模型分析结果表明:超临界甲烷吸附只能形成单层吸附,其中吸附相密度和绝对吸附量均随压力单调递增,吸附相体积近似保持不变。随着压力的升高,吸附相密度与气体相密度的差值先增加后减小,而吸附相体积近似保持不变,因此会导致过剩吸附量出现极大值。若将吸附相密度假定为定值会低估高压力段的绝对吸附量。

Kondo合金低温电阻率的自洽计算

从Slave-boson平均场理论出发,对Yoshimori-Kasai模型进行修正,应用相干势近似(CPA)方法计算了Kondo合金低温电阻率。结果表明,当合金中磁性原子浓度大于某个值时,重费米子系统明显地表现出相干性。给出了低温下电阻率的表达式。

基于Ono-Kondo格子模型的深部煤储层CH4吸附特征研究

为更准确研究深部煤储层煤层气的吸附特征,了解温度、压力、水等因素对煤层吸附CH4的影响,基于等温吸附实验,采用简化的Ono-Kondo格子模型的拟合方法,精确描述了4种煤级煤在不同温压条件下与不同流体作用前后的CH4等温吸附曲线。结果表明:压力会对CH4的吸附产生正效应,温度会对CH4的吸附产生负效应;压力越大,吸附量受温度影响程度越大;水分会降低煤对CH4的最大吸附容量,不利于CH4吸附;超临界CO2萃取作用,能够增大煤的微孔比表面积和孔体积,从而提高煤层CH4的最大吸附量;CH4的最大吸附量随煤级的变化呈现出"U"型关系。

AC Conductance Through a Vibrating Molecular Dot in Kondo Regime

In the present paper,by applying the Lang-Firsov canonical transformation and the so-called non-crossingapproximation technique,we investigate the joint effects of the electron-phonon interaction and an external alternatinggate voltage on the transport of a quantum dot system in the Kondo regime.We find that,while the satellite Kondoresonant peaks appear in both the averaged local density of states and the differential conductance,the main Kondopeak at the Fermi energy is greatly suppressed.These results confirm the previous ones derived by other methods,suchas the equation of motion solution.Furthermore,based on the picture of virtual transition between quasi-eigenstates inthe system,we also give a slightly different explanation on these phenomena.

Kondo effect for electron transport through an artificial quantum dot

We have calculated the transport properties of electron through an artificial quantum dot by using the numerical renormalization group technique in this paper. We obtain the conductance for the system of a quantum dot which is embedded in a one-dimensional chain in zero and finite temperature cases. The external magnetic field gives rise to a negative magnetoconductance in the zero temperature case. It increases as the external magnetic field increases, We obtain the relation between the coupling coefficient and conductance. If the interaction is big enough to prevent conduction electrons from tunnelling through the dot, the dispersion effect is dominant in this case. In the Kondo temperature regime, we obtain the conductivity of a quantum dot system with Kondo correlation.

Capacitive coupling induced Kondo–Fano interference in side-coupled double quantum dots

We report capacitive coupling induced Kondo–Fano(K–F) interference in a double quantum dot(DQD) by systematically investigating its low-temperature properties on the basis of hierarchical equations of motion evaluations. We show that the interdot capacitive coupling U12 splits the singly-occupied(S-O) state in quantum dot 1(QD1) into three quasi-particle substates: the unshifted S-O0 substate, and elevated S-O1 and S-O2. As U12 increases, S-O2 and S-O1 successively cross through the Kondo resonance state at the Fermi level(ω = 0), resulting in the so-called Kondo-I(KI), K–F, and Kondo-II(KII) regimes. While both the KI and KII regimes have the conventional Kondo resonance properties, remarkable Kondo–Fano interference features are shown in the K–F regime. In the view of scattering, we propose that the phase shift η(ω)is suitable for analysis of the Kondo–Fano interference. We present a general approach for calculating η(ω) and applying it to the DQD in the K–F regime where the two maxima of η(ω = 0) characterize the interferences between the Kondo resonance state and S-O2 and S-O1 substates, respectively.

Electric-Current-Induced Heat Generation in Kondo Regime

Using the nonequilibrium Green's function technique,we investigate the current induced heat generationin Kondo regime.The Kondo effect influences the heat generation significantly.In the curve of heat generation versusthe bias,a negative differential of the heat generation is exhibited.The symmetry of the heat generation is destroyed bythe strong electron-electron interaction and the electron-phonon interaction.

弱色散Kondo晶格模型

从s—f交换模型出发,在f带中引入弱色散项,讨论了重费米子系统正常态的低温特性。文中应用自洽场近似计算了低温磁化率和低温电阻率,结果表明,弱色散Kondo晶格模型能够解释重费米子系统的低温反常现象。

Coexistence of Quasi-two-dimensional Superconductivity and Tunable Kondo Lattice in a van der Waals Superconductor

Realization of Kondo lattice in superconducting van der Waals materials not only provides a unique opportunity for tuning the Kondo lattice behavior by electrical gating or intercalation,but also is helpful for further understanding the heavy fermion superconductivity.Here we report a low-temperature and vector-magneticfield scanning tunneling microscopy and spectroscopy study on a superconducting compound(4Hb-TaS_(2))with alternate stacking of 1T-TaS_(2)and 1H-TaS_(2)layers.We observe the quasi-two-dimensional superconductivity in the 1H-TaS_(2)layer with anisotropic response to the in-plane and out-of-plane magnetic fields.In the 1T-TaS_(2)layer,we detect the Kondo resonance peak that results from the Kondo screening of the unpaired electrons in the Star-of-David clusters.We also find that the intensity of the Kondo resonance peak is sensitive to its relative position with the Fermi level,and it can be significantly enhanced when it is further shifted towards the Fermi level by evaporating Pb atoms onto the 1T-TaS_(2)surface.Our results not only are important for fully understanding the electronic properties of 4Hb-TaS_(2),but also pave the way for creating tunable Kondo lattice in the superconducting van der Waals materials.

基于Kondo粒子散射的电子自旋纠缠

通过研究自旋不固定的Kondo粒子散射对电子自旋状态的影响,可为调控电子自旋的纠缠程度以及量子信息传递提供理论基础。文章基于Kondo粒子散射理论模型,分别研究了Kondo粒子散射对单自由电子和双自由电子自旋纠缠程度的影响,利用Mathematica软件计算了纠缠度的变化特征。结果表明:当自由电子经过时,Kondo粒子散射改变了入射电子态中不同成分自旋的比例,起到了纠缠浓缩的作用;当相互作用的2个自由电子经过时,Kondo粒子散射可以使其形成自旋纠缠,其纠缠程度取决于初始状态和散射势高度,适当调整势垒高度能够有效地控制电子纠缠程度。

Magnetoresistance hysteresis in topological Kondo insulator SmB6 nanowire

SmB6, a topological Kondo insulator, with a gapped bulk state and metallic surface state has aroused great research interest. Here, we report an exotic hysteresis behavior of magnetoresistance in individual SmB6 nanowire in a temperature range in which both surface and bulk states contribute to the total conductance. Under a magnetic field parallel to the SmB6 nanowire, the resistance suddenly increases at the turning point from up-sweep to down-sweep of the magnetic field. The magnetoresistance hysteresis loops are well consistent with the magnetocaloric effect. Our results suggest that the SmB6 nanowires possess potential applications in the magnetic cooling technology.

Global phase diagram of a spin–orbit-coupled Kondo lattice model on the honeycomb lattice

Motivated by the growing interest in the novel quantum phases in materials with strong electron correlations and spin–orbit coupling, we study the interplay among the spin–orbit coupling, Kondo interaction, and magnetic frustration of a Kondo lattice model on a two-dimensional honeycomb lattice.We calculate the renormalized electronic structure and correlation functions at the saddle point based on a fermionic representation of the spin operators.We find a global phase diagram of the model at half-filling, which contains a variety of phases due to the competing interactions.In addition to a Kondo insulator, there is a topological insulator with valence bond solid correlations in the spin sector, and two antiferromagnetic phases.Due to the competition between the spin–orbit coupling and Kondo interaction, the direction of the magnetic moments in the antiferromagnetic phases can be either within or perpendicular to the lattice plane.The latter antiferromagnetic state is topologically nontrivial for moderate and strong spin–orbit couplings.

Transition from the Kondo effect to a Coulomb blockade in an electron shuttle

We investigate the effect of the mechanical motion of a quantum dot on the transport properties of a quantum dot shuttle, Employing the equation of motion method for the nonequilibrium Green＇s function, we show that the oscillation of the dot, i.e., the time-dependent coupling between the dot＇s electron and the reservoirs, can destroy the Kondo effect. With the increase in the oscillation frequency of the dot, the density of states of the quantum dot shuttle changes from the Kondo-like to a Coulomb-blockade pattern. Increasing the coupling between the dot and the electrodes may partly recover the Kondo peak in the spectrum of the density of states. Understanding of the effect of mechanical motion on the transport properties of an electron shuttle is important for the future application of nanoelectromechanical devices.

Kondo effect in a deformed molecule coupled asymmetrically to ferromagnetic electrodes

The nonequilibrium Kondo effect is studied in a molecule quantum dot coupled asymmetrically to two ferromagnetic electrodes by employing the nonequilibrium Green function technique. The current-induced deformation of the molecule is taken into account, modeled as interactions with a phonon system, and phonon-assisted Kondo satellites arise on both sides of the usual main Kondo peak. In the antiparallel electrode configuration, the Kondo satellites can be split only for the asymmetric dot-lead couplings, distinguished from the parallel configuration where splitting also exists, even though it is for symmetric case. We also analyze how to compensate the splitting and restore the suppressed zero-bias Kondo resonance. It is shown that one can change the TMR ratio significantly from a negative dip to a positive peak only by slightly modulating a local external magnetic field, whose value is greatly dependent on the electron-phonon coupling strength.

Giant Kondo Resonance of Parallel-Coupled Double Quantum Dots Embedded in an A-B Ring

We theoretically study the properties of the ground state of the parallel-coupled double quantum dots embedded in a mesoscopic ring in the Kondo regime by means of the two-impurity Anderson Hamiltonian. The Hamiltonian is solved by means of the slave-boson mean-field theory. We find that in this system, the persistent current depends sensitively on both the parity of this system and the size of the ring. In the strong coupling regime, the giant sharp current peak appears, at the same time, the parity dependence of the persistent current disappears. These imply that in the strong coupling regime, there exists giant Kondo resonance and the two dots can be coupled coherently. Thus this system might be a candidate for future device applications.