1,660 research outputs found
Suppression of Kondo effect in a quantum dot by external irradiation
We demonstrate that the external irradiation brings decoherence in the spin
states of the quantum dot. This effect cuts off the Kondo anomaly in
conductance even at zero temperature. We evaluate the dependence of the DC
conductance in the Kondo regime on the power of irradiation, this dependence
being determined by the decoherence.Comment: 4 pages, 1 figur
The Kondo Effect in Non-Equilibrium Quantum Dots: Perturbative Renormalization Group
While the properties of the Kondo model in equilibrium are very well
understood, much less is known for Kondo systems out of equilibrium. We study
the properties of a quantum dot in the Kondo regime, when a large bias voltage
V and/or a large magnetic field B is applied. Using the perturbative
renormalization group generalized to stationary nonequilibrium situations, we
calculate renormalized couplings, keeping their important energy dependence. We
show that in a magnetic field the spin occupation of the quantum dot is
non-thermal, being controlled by V and B in a complex way to be calculated by
solving a quantum Boltzmann equation. We find that the well-known suppression
of the Kondo effect at finite V>>T_K (Kondo temperature) is caused by inelastic
dephasing processes induced by the current through the dot. We calculate the
corresponding decoherence rate, which serves to cut off the RG flow usually
well inside the perturbative regime (with possible exceptions). As a
consequence, the differential conductance, the local magnetization, the spin
relaxation rates and the local spectral function may be calculated for large
V,B >> T_K in a controlled way.Comment: 9 pages, invited paper for a special edition of JPSJ "Kondo Effect --
40 Years after the Discovery", some typos correcte
Theory of the Fano Resonance in the STM Tunneling Density of States due to a Single Kondo Impurity
The conduction electron density of states nearby single magnetic impurities,
as measured recently by scanning tunneling microscopy (STM), is calculated,
taking into account tunneling into conduction electron states only. The Kondo
effect induces a narrow Fano resonance in the conduction electron density of
states, while scattering off the d-level generates a weakly energy dependent
Friedel oscillation. The line shape varies with the distance between STM tip
and impurity, in qualitative agreement with experiments, but is very sensitive
to details of the band structure. For a Co impurity the experimentally observed
width and shift of the Kondo resonance are in accordance with those obtained
from a combination of band structure and strongly correlated calculations.Comment: 4 pages, ReVTeX + 4 figures (Encapsulated Postscript), submitted to
PR
Quantum dots with even number of electrons: Kondo effect in a finite magnetic field
We study a small spin-degenerate quantum dot with even number of electrons,
weakly connected by point contacts to the metallic electrodes, and subject to
an external magnetic field. If the Zeeman energy B is equal to the
single-particle level spacing in the dot, the ground state of the dot
becomes doubly degenerate, and the system exhibits Kondo effect, despite the
fact that B exceeds by far the Kondo temperature . A possible
realization of this in tunneling experiments is discussed
Spin-charge separation and Kondo effect in an open quantum dot
We study a quantum dot connected to the bulk by single-mode junctions at
almost perfect conductance. Although the average charge of
the dot is not discrete, its spin remains quantized: or ,
depending (periodically) on the gate voltage. This drastic difference from the
conventional mixed-valence regime stems from the existence of a broad-band,
dense spectrum of discrete levels in the dot. In the doublet state, the Kondo
effect develops at low temperatures. We find the Kondo temperature and
the conductance at .Comment: 4 pages, 1 figur
Equation of motion approach to the solution of Anderson model
Based on an equation of motion approach the single impurity Anderson
model(SIAM) is reexamined. Using the cluster expansions the equations of motion
of Green functions are transformed into the corresponding equations of motion
of connected Green functions, which provides a natural and uniform truncation
scheme. A factor of two missing in the Lacroix's approximation for the Kondo
temperature is gained in the next higher order truncation beyond Lacroix's. A
quantitative improvement in the density of states at the Fermi level is also
obtained.Comment: 4 pages, 2 figure
A Self-Consistent First-Principles Technique Having Linear Scaling
An algorithm for first-principles electronic structure calculations having a
computational cost which scales linearly with the system size is presented. Our
method exploits the real-space localization of the density matrix, and in this
respect it is related to the technique of Li, Nunes and Vanderbilt. The density
matrix is expressed in terms of localized support functions, and a matrix of
variational parameters, L, having a finite spatial range. The total energy is
minimized with respect to both the support functions and the elements of the L
matrix. The method is variational, and becomes exact as the ranges of the
support functions and the L matrix are increased. We have tested the method on
crystalline silicon systems containing up to 216 atoms, and we discuss some of
these results.Comment: 12 pages, REVTeX, 2 figure
Exact non-equilibrium current from the partition function for impurity transport problems
We study the partition functions of quantum impurity problems in the domain
of complex applied bias for its relation to the non-equilibrium current
suggested by Fendley, Lesage and Saleur (cond-mat/9510055). The problem is
reformulated as a certain generalization of the linear response theory that
accomodates an additional complex variable. It is shown that the mentioned
relation holds in a rather generic case in the linear response limit, or under
certain condition out of equilibrium. This condition is trivially satisfied by
the quadratic Hamiltonians and is rather restrictive for the interacting
models. An example is given when the condition is violated.Comment: 10 pages, RevTex. Final extended versio
Spin-orbit Scattering and the Kondo Effect
The effects of spin-orbit scattering of conduction electrons in the Kondo
regime are investigated theoretically. It is shown that due to time-reversal
symmetry, spin-orbit scattering does not suppress the Kondo effect, even though
it breaks spin-rotational symmetry, in full agreement with experiment. An
orbital magnetic field, which breaks time-reversal symmetry, leads to an
effective Zeeman splitting, which can be probed in transport measurements. It
is shown that, similar to weak-localization, this effect has anomalous magnetic
field and temperature dependence.Comment: 10 pages, RevTex, one postscript figure available on request from
[email protected]
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