113 research outputs found
Magnetically Tunable Kondo - Aharonov-Bohm Effect in a Triangular Quantum Dot
The role of discrete orbital symmetry in mesoscopic physics is manifested in
a system consisting of three identical quantum dots forming an equilateral
triangle. Under a perpendicular magnetic field, this system demonstrates a
unique combination of Kondo and Aharonov-Bohm features due to an interplay
between continuous [spin-rotation SU(2)] and discrete (permutation C3v)
symmetries, as well as U(1) gauge invariance. The conductance as a function of
magnetic flux displays sharp enhancement or complete suppression depending on
contact setups.Comment: 4 pages, 3 .eps figure
Kondo Lattice without Nozieres Exhaustion Effect
We discuss the properties of layered Anderson/Kondo lattices with metallic
electrons confined in 2D xy planes and local spins in insulating layers forming
chains in z direction. Each spin in this model possesses its own 2D Kondo
cloud, so that the Nozieres' exhaustion problem does not occur. The excitation
spectrum of the model is gapless both in charge and spin sectors. The
disordered phases and possible experimental realizations of the model are
briefly discussed.Comment: 4 pages, 3 figure
Interplay between Heavy Fermions and Crystal Field Excitation in Kondo Lattices. Low-Temperature Thermodynamics and Inelastic Neutron Scattering Spectra of CeNiSn
The microscopic theory of interaction between the heavy fermions and the
crystal field excitations in Kondo lattices is presented. It is shown that the
heavy-fermion spectrum scaled by the Kondo temperature can be modified by
the crystal field excitations with the energy provided the
inequality is realized. On the base of general description of
excitation spectrum the detailed qualitative and quantitative explanation of
anisotropic inelastic neutron scattering spectra and low-temperature specific
heat of orthorhombic CeNiSn is given. The theory resolves the apparent
contradiction between the metallic conductivity and the gap-wise behavior of
thermodynamic properties and spin response of CeNiSn at low temperatures.Comment: 24 pages (LaTeX), 12 Postscript figures, submitted to Phys.Rev.
Electron self-trapping in intermediate-valent SmB6
SmB6 exhibits intermediate valence in the ground state and unusual behaviour
at low temperatures. The resistivity and the Hall effect cannot be explained
either by conventional sf-hybridization or by hopping transport in an impurity
band. At least three different energy scales determine three temperature
regimes of electron transport in this system. We consider the ground state
properties, the soft valence fluctuations and the spectrum of band carriers in
n-doped SmB6. The behaviour of excess conduction electrons in the presence of
soft valence fluctuations and the origin of the three energy scales in the
spectrum of elementary excitations is discussed. The carriers which determine
the low-temperature transport in this system are self-trapped electron-polaron
complexes rather than simply electrons in an impurity band. The mechanism of
electron trapping is the interaction with soft valence fluctuations.Comment: 12 pages, 3 figure
Superexchange in Dilute Magnetic Dielectrics: Application to (Ti,Co)O_2
We extend the model of ferromagnetic superexchange in dilute magnetic
semiconductors to the ferromagnetically ordered highly insulating compounds
(dilute magnetic dielectrics). The intrinsic ferromagnetism without free
carriers is observed in oxygen-deficient films of anatase TiO_2 doped with
transition metal impurities in cation sublattice. We suppose that ferromagnetic
order arises due to superexchange between complexes [oxygen vacancies +
magnetic impurities], which are stabilized by charge transfer from vacancies to
impurities. The Hund rule controls the superexchange via empty vacancy related
levels so that it becomes possible only for the parallel orientation of
impurity magnetic moments. The percolation threshold for magnetic ordering is
determined by the radius of vacancy levels, but the exchange mechanism does not
require free carriers. The crucial role of the non-stoichiometry in formation
of the ferromagnetism makes the Curie temperatures extremely sensitive to the
methods of sample preparation.Comment: 18 pages, 2 figure
Kondo effect in systems with dynamical symmetries
This paper is devoted to a systematic exposure of the Kondo physics in
quantum dots for which the low energy spin excitations consist of a few
different spin multiplets . Under certain conditions (to be
explained below) some of the lowest energy levels are nearly
degenerate. The dot in its ground state cannot then be regarded as a simple
quantum top in the sense that beside its spin operator other dot (vector)
operators are needed (in order to fully determine its quantum
states), which have non-zero matrix elements between states of different spin
multiplets . These "Runge-Lenz"
operators do not appear in the isolated dot-Hamiltonian (so in some sense they
are "hidden"). Yet, they are exposed when tunneling between dot and leads is
switched on. The effective spin Hamiltonian which couples the metallic electron
spin with the operators of the dot then contains new exchange terms,
beside the ubiquitous ones . The operators and generate a
dynamical group (usually SO(n)). Remarkably, the value of can be controlled
by gate voltages, indicating that abstract concepts such as dynamical symmetry
groups are experimentally realizable. Moreover, when an external magnetic field
is applied then, under favorable circumstances, the exchange interaction
involves solely the Runge-Lenz operators and the corresponding
dynamical symmetry group is SU(n). For example, the celebrated group SU(3) is
realized in triple quantum dot with four electrons.Comment: 24 two-column page
On the validity of the Franck-Condon principle in the optical spectroscopy: optical conductivity of the Fr\"{o}hlich polaron
The optical absorption of the Fr\"{o}hlich polaron model is obtained by an
approximation-free Diagrammatic Monte Carlo method and compared with two new
approximate approaches that treat lattice relaxation effects in different ways.
We show that: i) a strong coupling expansion, based on the the Franck-Condon
principle, well describes the optical conductivity for large coupling strengths
(); ii) a Memory Function Formalism with phonon broadened levels
reproduces the optical response for weak coupling strengths ()
taking the dynamic lattice relaxation into account. In the coupling regime
the optical conductivity is a rapidly changing superposition of
both Franck-Condon and dynamic contributions.Comment: accepted for publication in PR
Resonance Kondo Tunneling through a Double Quantum Dot at Finite Bias
It is shown that the resonance Kondo tunneling through a double quantum dot
(DQD) with even occupation and singlet ground state may arise at a strong bias,
which compensates the energy of singlet/triplet excitation. Using the
renormalization group technique we derive scaling equations and calculate the
differential conductance as a function of an auxiliary dc-bias for parallel DQD
described by SO(4) symmetry. We analyze the decoherence effects associated with
the triplet/singlet relaxation in DQD and discuss the shape of differential
conductance line as a function of dc-bias and temperature.Comment: 11 pages, 6 eps figures include
- …