192,957 research outputs found
Microscopic mechanisms of magnetization reversal
Two principal scenarios of magnetization reversal are considered. In the
first scenario all spins perform coherent motion and an excess of magnetic
energy directly goes to a nonmagnetic thermal bath. A general dynamic equation
is derived which includes a tensor damping term similar to the
Bloch-Bloembergen form but the magnetization magnitude remains constant for any
deviation from equilibrium. In the second reversal scenario, the absolute value
of the averaged sample magnetization is decreased by a rapid excitation of
nonlinear spin-wave resonances by uniform magnetization precession. We have
developed an analytic k-space micromagnetic approach that describes this entire
reversal process in an ultra-thin soft ferromagnetic film for up to 90^{o}
deviation from equilibrium. Conditions for the occurrence of the two scenarios
are discussed
Atomic structure of Ge quantum dots on the Si(001) surface
In situ morphological investigation of the {105} faceted Ge islands on the
Si(001) surface (hut clusters) have been carried out using an ultra high vacuum
instrument integrating a high resolution scanning tunnelling microscope and a
molecular beam epitaxy vessel. Both species of hut clusters--pyramids and
wedges--were found to have the same structure of the {105} facets which was
visualized. Structures of vertexes of the pyramidal clusters and ridges of the
wedge-shaped clusters were revealed as well and found to be different. This
allowed us to propose a crystallographic model of the {105} facets as well as
models of the atomic structure of both species of the hut clusters. An
inference is made that transitions between the cluster shapes are impossible.Comment: 6 pages, 6 figures. Accepted to JETP Letters (publication date
2010-03-25
Negative differential thermal resistance and thermal transistor
We report on the first model of a thermal transistor to control heat flow.
Like its electronic counterpart, our thermal transistor is a three-terminal
device with the important feature that the current through the two terminals
can be controlled by small changes in the temperature or in the current through
the third terminal. This control feature allows us to switch the device between
"off" (insulating) and "on" (conducting) states or to amplify a small current.
The thermal transistor model is possible because of the negative differential
thermal resistance.Comment: 4 pages, 4 figures. SHortened. To appear in Applied Physics Letter
Flow Vorticity in Peripheral High Energy Heavy Ion Collisions
The vorticity development is studied in the reaction plane of peripheral
relativistic heavy ion reactions where the initial state has substantial
angular momentum. The earlier predicted rotation effect and Kelvin Helmholtz
Instability, lead to significant initial vorticity and circulation. In low
viscosity QGP this vorticity remains still significant at the time of freeze
out of the system, even if damping due to the explosive expansion and the
dissipation decreases the vorticity and circulation. In the reaction plane the
vorticity arises from the initial angular momentum, and it is stronger than in
the transverse plane where vorticity is caused by random fluctuations only
Implementation of universal quantum gates based on nonadiabatic geometric phases
We propose an experimentally feasible scheme to achieve quantum computation
based on nonadiabatic geometric phase shifts, in which a cyclic geometric phase
is used to realize a set of universal quantum gates. Physical implementation of
this set of gates is designed for Josephson junctions and for NMR systems.
Interestingly, we find that the nonadiabatic phase shift may be independent of
the operation time under appropriate controllable conditions. A remarkable
feature of the present nonadiabatic geometric gates is that there is no
intrinsic limitation on the operation time, unlike adiabatic geometric gates.
Besides fundamental interest, our results may simplify the implementation of
geometric quantum computation based on solid state systems, where the
decoherence time may be very short.Comment: 5 pages, 2 figures; the version published in Phys. Rev. Let
Modified Fragmentation Function from Quark Recombination
Within the framework of the constituent quark model, it is shown that the
single hadron fragmentation function of a parton can be expressed as a
convolution of shower diquark or triquark distribution function and quark
recombination probability, if the interference between amplitudes of quark
recombination with different momenta is neglected. The recombination
probability is determined by the hadron's wavefunction in the constituent quark
model. The shower diquark or triquark distribution functions of a fragmenting
jet are defined in terms of overlapping matrices of constituent quarks and
parton field operators. They are similar in form to dihadron or trihadron
fragmentation functions in terms of parton operator and hadron states.
Extending the formalism to the field theory at finite temperature, we
automatically derive contributions to the effective single hadron fragmentation
function from the recombination of shower and thermal constituent quarks. Such
contributions involve single or diquark distribution functions which in turn
can be related to diquark or triquark distribution functions via sum rules. We
also derive QCD evolution equations for quark distribution functions that in
turn determine the evolution of the effective jet fragmentation functions in a
thermal medium.Comment: 23 pages in RevTex with 8 postscript figure
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