6,030 research outputs found
Non-Markovian dynamics with fermions
Employing the quadratic fermionic Hamiltonians for the collective and
internal subsystems with a linear coupling, we studied the role of fermionic
statistics on the dynamics of the collective motion. The transport coefficients
are discussed as well as the associated fluctuation-dissipation relation. Due
to different nature of the particles, the path to equilibrium is slightly
affected. However, in the weak coupling regime, the time-scale for approaching
equilibrium is found to be globally unchanged. The Pauli-blocking effect can
modify the usual picture in open quantum system. In some limits, contrary to
boson, this effect can strongly hinder the influence of the bath by blocking
the interacting channels.Comment: 13 pages, 6 figures. Submitted to PR
Neutron pair transfer in sub-barrier capture process
The sub-barrier capture reactions following the neutron pair transfer are
proposed to be used for the indirect study of neutron-neutron correlation in
the surface region of nucleus. The strong effect of the dineutron-like clusters
transfer stemming from the surface of magic and non-magic nuclei O,
Ca, Ni, Mo, Ru, Pd, and
Sn is demonstrated. The dominance of
two-neutron transfer channel at the vicinity of the Coulomb barrier is further
supported by time-dependent mean-field approaches.Comment: 17 pages, 7 figures, accepted in PR
Magnetic blackbody shift of hyperfine transitions for atomic clocks
We derive an expression for the magnetic blackbody shift of hyperfine
transitions such as the cesium primary reference transition which defines the
second. The shift is found to be a complicated function of temperature, and has
a T^2 dependence only in the high-temperature limit. We also calculate the
shift of ground-state p_1/2 hyperfine transitions which have been proposed as
new atomic clock transitions. In this case interaction with the p_3/2
fine-structure multiplet may be the dominant effect
Polarization of the nuclear surface in deformed nuclei
The density profiles of around 750 nuclei are analyzed using the Skyrme
energy density functional theory. Among them, more than 350 nuclei are found to
be deformed. In addition to rather standard properties of the density, we
report a non-trivial behavior of the nuclear diffuseness as the system becomes
more and more deformed. Besides the geometric effects expected in rigid body,
the diffuseness acquires a rather complex behavior leading to a reduction of
the diffuseness along the main axis of deformation simultaneously with an
increase of the diffuseness along the other axis. The possible isospin
dependence of this polarization is studied. This effect, that is systematically
seen in medium- and heavy-nuclei, can affect the nuclear dynamical properties.
A quantitative example is given with the fusion barrier in the Ca+
U reaction.Comment: 8 pages, 13 figure
Graphene in periodically alternating magnetic field: unusual quantization of the anomalous Hall effect
We study the energy spectrum and electronic properties of graphene in a
periodic magnetic field of zero average with a symmetry of triangular lattice.
The periodic field leads to formation of a set of minibands separated by gaps,
which can be manipulated by external field. The Berry phase, related to the
motion of electrons in space, and the corresponding Chern numbers
characterizing topology of the energy bands are calculated analytically and
numerically. In this connection, we discuss the anomalous Hall effect in the
insulating state, when the Fermi level is located in the minigap. The results
of calculations show that in the model of gapless Dirac spectrum of graphene
the anomalous Hall effect can be treated as a sum of fractional quantum
numbers, related to the nonequivalent Dirac points.Comment: 6 pages, 5 figure
Anomalous Hall Effect due to the spin chirality in the Kagom\'{e} lattice
We consider a model for a two dimensional electron gas moving on a kagom\'{e}
lattice and locally coupled to a chiral magnetic texture. We show that the
transverse conductivity does not vanish even if spin-orbit
coupling is not present and it may exhibit unusual behavior. Model parameters
are the chirality, the number of conduction electrons and the amplitude of the
local coupling. Upon varying these parameters, a topological transition
characterized by change of the band Chern numbers occur. As a consequence,
can be quantized, proportional to the chirality or have a non
monotonic behavior upon varying these parameters.Comment: 8 pages, 7 figure
Berry phase of magnons in textured ferromagnets
We study the energy spectrum of magnons in a ferromagnet with topologically
nontrivial magnetization profile. In the case of inhomogeneous magnetization
corresponding to a metastable state of ferromagnet, the spin-wave equation of
motion acquires a gauge potential leading to a Berry phase for the magnons
propagating along a closed contour. The effect of magnetic anisotropy is
crucial for the Berry phase: we show that the anisotropy suppresses its
magnitude, which makes the Berry phase observable in some cases, similar to the
Aharonov-Bohm effect for electrons. For example, it can be observed in the
interference of spin waves propagating in mesoscopic rings. We discuss the
effect of domain walls on the interference in ferromagnetic rings, and propose
some experiments with a certain geometry of magnetization. We also show that
the nonvanishing average topological field acts on the magnons like a uniform
magnetic field on electrons. It leads to the quantization of the magnon
spectrum in the topological field.Comment: 8 pages, 5 figure
Chiral two-dimensional electron gas in a periodic magnetic field
We study the energy spectrum and electronic properties of two-dimensional
electron gas in a periodic magnetic field of zero average with a symmetry of
triangular lattice. We demonstrate how the structure of electron energy bands
can be changed with the variation of the field strength, so that we can start
from nearly free electron gas and then transform it continuously to a system of
essentially localized chiral electron states. We find that the electrons near
some minima of the effective potential are responsible for occurrence of
dissipationless persistent currents creating a lattice of current contours. The
topological properties of the electron energy bands are also varied with the
intensity of periodic field. We calculated the topological Chern numbers of
several lower energy bands as a function of the field. The corresponding Hall
conductivity is nonzero and, when the Fermi level lies in the gap, it is
quantized.Comment: 10 pages;9 figures;42 reference
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