175 research outputs found

    Anomalous magnetic splitting of the Kondo resonance

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    The splitting of the Kondo resonance in the density of states of an Anderson impurity in finite magnetic field is calculated from the exact Bethe-ansatz solution. The result gives an estimate of the electron spectral function for nonzero magnetic field and Kondo temperature, with consequences for transport experiments on quantum dots in the Kondo regime. The strong correlations of the Kondo ground state cause a significant low-temperature reduction of the peak splitting. Explicit formulae are found for the shift and broadening of the Kondo peaks. A likely cause of the problems of large-N approaches to spin-1/2 impurities at finite magnetic field is suggested.Comment: 4 pages, 2 eps figures; published versio

    Ground State and Spectral Properties of a Quantum Impurity in d-Wave Superconductors

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    The variational approach of Gunnarsson and Sch\"onhammer to the Anderson impurity model is generalized to study d-wave superconductors in the presence of dilute spin-1/2 impurities. We show that the local moment is screened when the hybridization exceeds a nonzero critical value at which the ground state changes from a spin doublet to a spin singlet. The electron spectral functions are calculated in both phases. We find that while a Kondo resonance develops above the Fermi level in the singlet phase, the spectral function exhibits a low-energy spectral peak below the Fermi level in the spin doublet phase. The origin of such a ``virtual Kondo resonance'' is the existence of low-lying collective excitations in the spin-singlet sector. We discuss our results in connection to recent spectroscopic experiments on Zn doped high-Tc_c superconductors.Comment: 5 pages, 4figures, revised versio

    Non Fermi Liquid Behaviour near a T=0T=0 spin-glass transition

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    In this paper we study the competition between the Kondo effect and RKKY interactions near the zero-temperature quantum critical point of an Ising-like metallic spin-glass. We consider the mean-field behaviour of various physical quantities. In the `quantum- critical regime' non-analytic corrections to the Fermi liquid behaviour are found for the specific heat and uniform static susceptibility, while the resistivity and NMR relaxation rate have a non-Fermi liquid dependence on temperature.Comment: 15 pages, RevTex 3.0, 1 uuencoded ps. figure at the en

    Nonvanishing Local Moment in Triplet Superconductors

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    The Kondo effect in a px+ipyp_x + {\rm i} p_y-wave superconductor is studied by applying the Wilson's numerical renormalization group method. In this type of superconductor with a full energy gap like a s-wave one, the ground state is always a spin doublet, while a local spin is shrunk by the Kondo effect. The calculated magnetic susceptibility indicates that the spin of the ground state is generated by the orbital effect of the px+ipyp_x + {\rm i} p_y-wave Cooper pairs. The effect of spin polarization of the triplet superconductor is also discussed.Comment: 5 pages, 4 figures, to be published in J. Phys. Soc. Jp

    Bethe ansatz approach to thermodynamics of superconducting magnetic alloys

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    We derive thermodynamic Bethe ansatz equations for a model describing an UU\to\infty Anderson impurity embedded in a BCS superconductor. The equations are solved analytically in the zero-temperature limit, T=0. It is shown that the impurities depress superconductivity in the Kondo limit, however at T=0 the system remains in the superconducting state for any impurity concentration. In the mixed-valence regime, an impurity contribution to the density of states of the system near the Fermi level overcompensates a Cooper pairs weakening, and superconductivity is enhanced.Comment: 4 pages, RevTex, to appear in PR

    Multichannel pseudogap Kondo model: Large-N solution and quantum-critical dynamics

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    We discuss a multichannel SU(N) Kondo model which displays non-trivial zero-temperature phase transitions due to a conduction electron density of states vanishing with a power law at the Fermi level. In a particular large-N limit, the system is described by coupled integral equations corresponding to a dynamic saddle point. We exactly determine the universal low-energy behavior of spectral densities at the scale-invariant fixed points, obtain anomalous exponents, and compute scaling functions describing the crossover near the quantum-critical points. We argue that our findings are relevant to recent experiments on impurity-doped d-wave superconductors.Comment: 4 pages, 3 figs; extended discussion of large-N spin representations, added references; accepted for publication in PR

    Exactly solvable toy models of unconventional magnetic alloys: Bethe Ansatz versus Renormalization Group method

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    We propose toy models of unconventional magnetic alloys, in which the density of band states, ρ(ϵ)\rho(\epsilon), and hybridization, t(ϵ)t(\epsilon), are energy dependent; it is assumed, however, that t2(ϵ)ρ1(ϵ)t^2(\epsilon)\propto\rho^{-1}(\epsilon), and hence an effective electron-impurity coupling Γ(ϵ)=ρ(ϵ)t2(ϵ)\Gamma(\epsilon)=\rho(\epsilon)t^2(\epsilon) is energy independent. In the renormalization group approach, the physics of the system is assumed to be governed by Γ(ϵ)\Gamma(\epsilon) only rather than by separate forms of ρ(ϵ)\rho(\epsilon) and t(ϵ)t(\epsilon). However, an exact Bethe Ansatz solution of the toy Anderson model demonstrates a crucial role of a form of inverse band dispersion k(ϵ)k(\epsilon).Comment: A final version. A previous one has been sent to Archive because of my technical mistake. Sorr

    Overscreening of magnetic impurities in dx2y2d_{x^2-y^2} wave superconductors

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    We consider the screening of a magnetic impurity in a dx2y2d_{x^2-y^2} wave superconductor. The properties of the dx2y2d_{x^2-y^2} state lead to an unusual behavior in the impurity magnetic susceptibility, the impurity specific heat and in the quasiparticle phase shift which can be used to diagnose the nature of the condensed state. We construct an effective theory for this problem and show that it is equivalent to a multichannel (one per node) non-marginal Kondo problem with linear density of states and coupling constant J. There is a quantum phase transition from an unscreened impurity state to an overscreened Kondo state at a critical value J_c which varies with Δ0\Delta_0, the superconducting gap away from the nodes. In the overscreened phase, the impurity Fermi level ϵf\epsilon_f and the amplitude Δ\Delta of the ground state singlet vanish at J_c like Δ0exp(const./Δ)\Delta_0 \exp(- const. / \Delta) and J-J_c respectively. We derive the scaling laws for the susceptibility and specific heat in the overscreened phase at low fields and temperatures.Comment: 43 pages; shortened version; a number of typos have been correcte

    Persistence of Li Induced Kondo Moments in the Superconducting State of Cuprates

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    We measure the magnetic susceptibility nearby Li spinless impurities in the superconducting phase of the high Tc cuprate YBaCuO. The induced moment which was found to exist above Tc persists below Tc. In the underdoped regime, it retains its Curie law below Tc. In contrast, near optimal doping, the large Kondo screening observed above Tc (T_K=135 K) is strongly reduced below Tc as expected theoretically when the superconducting gap develops. This moment still extends essentially on its 4 near neighbour Cu, showing the persistence of AF correlations in the superconducting state. A direct comparison with recent STM results of Pan et al. is proposed.Comment: accepted for publication in Phys. Rev. Lett. (issue of 30 april 2001) Revised version : 8 pages including 4 pages of text and 4 figure

    Kondo screening in d-wave superconductors in a Zeeman field and implications for STM spectra of Zn-doped cuprates

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    We consider the screening of an impurity moment in a d-wave superconductor under the influence of a Zeeman magnetic field. Using the Numerical Renormalization Group technique, we investigate the resulting pseudogap Kondo problem, in particular the field-induced crossover behavior in the vicinity of the zero-field boundary quantum phase transition. The impurity spectral function and the resulting changes in the local host density of states are calculated, giving specific predictions for high-field STM measurements on impurity-doped cuprates.Comment: 5 pages, 4 figs, (v2) remark on c-axis field added, discussion extended, (v3) final version as publishe
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