1,690 research outputs found
Extraordinary SEAWs under influence of the spin-spin interaction and the quantum Bohm potential
The separate spin evolution (SSE) of electrons causes the existence of the
spin-electron acoustic wave. Extraordinary spin-electron acoustic waves (SEAWs)
propagating perpendicular to the external magnetic field have large
contribution of the transverse electric field. Its spectrum has been studied in
the quasi-classical limit at the consideration of the separate spin evolution.
The spin-spin interaction and the quantum Bohm potential give contribution in
the spectrum extraordinary SEAW. This contribution is studied in this paper.
Moreover, it is demonstrated that the spin-spin interaction leads to the
existence of the extraordinary SEAWs if the SSE is neglected. The hybridization
of the extraordinary SEAW and the lower extraordinary wave in the regime, where
the cyclotron frequency is larger then the Langmuir frequency is studied
either.Comment: 8 pages, 8 figure
Spin current contribution in the spectrum of collective excitations of degenerate partially polarized spin-1/2 fermions at separate dynamics of spin-up and spin-down fermions
The spectrum of collective excitations of degenerate partially polarized
spin-1/2 fermions is considered. The spin-up fermions and the spin-down
fermions are considered as different fluids. Corresponding two-fluid
hydrodynamics consistent with a non-linear Pauli equation is suggested. An
equation of state for the spin current caused by the distribution of particles
on different energy levels is suggested for the degenerate regime, where the
spin current is caused by the Pauli blocking. Spectrum of three waves is found
as a solution of the hydrodynamic equations: two sound waves and one spin wave.
Their spectrums are calculated for two regimes: propagation parallel and
perpendicular to the direction of the equilibrium spin polarization.Comment: 14 pages, 15 figure
Quantum hydrodynamic theory of quantum fluctuations in dipolar Bose-Einstein condensate
Traditional quantum hydrodynamics of Bose-Einstein condensates (BECs) is
restricted by the continuity and Euler equations. It corresponds to the
well-known Gross-Pitaevskii equation. However, the quantum Bohm potential,
which is a part of the momentum flux, has a nontrivial part with can evolve
under the quantum fluctuations. To cover this phenomenon in terms of
hydrodynamic methods we need to derive equations for the momentum flux, and the
third rank tensor. In all equations we consider the main contribution of the
short-range interaction (SRI) in the first order by the interaction radius.
Derived hydrodynamics consists of four hydrodynamic equations. The third moment
evolution equation contains interaction leading to the quantum fluctuations. It
includes new interaction constant. The Gross-Pitaevskii interaction constant is
the integral of potential, but the second interaction constant is the integral
of second derivative of potential. If we have dipolar BECs we deal with a
long-range interaction. Its contribution is proportional to the potential of
dipole-dipole interaction (DDI). The Euler equation contains the derivative of
the potential. The third rank tensor evolution equation contains the third
derivative of the potential. The quantum fluctuations lead to existence of the
second wave solution. Moreover, the quantum fluctuations introduce the
instability of BECs. If the DDI is attractive, but being smaller then the
repulsive SRI presented by the first interaction constant, there is the
long-wavelength instability. For the repulsive DDI these is more complex
picture. There is the small area with the long-wavelength instability which
transits into stability interval, where two waves exist. There is the
short-wavelength instability as well. These results are found for the DDI
strength comparable with the Gross-Pitaevskii SRI.Comment: 6+3 pages, 3+2 figure
Non-integral form of the Gross-Pitaevskii equation for polarized molecules
The Gross-Pitaevskii equation for polarized molecules is an
integro-differential equation, consequently it is complicated for solving. We
find a possibility to represent it as a non-integral nonlinear Schrodinger
equation, but this equation should be coupled with two linear equations
describing electric field. These two equations are the Maxwell equations. We
recapture the dispersion of collective excitations in the three dimensional
electrically polarized BEC with no evolution of the electric dipole moment
directions. We trace the contribution of the electric dipole moment. We
explicitly consider the contribution of the electric dipole moment in the
interaction constant for the short-range interaction. We show that the spectrum
of dipolar BEC reveals no instability at repulsive short-range interaction.
Nonlinear excitations are also considered. We present dependence of the bright
soliton characteristics on the electric dipole moment.Comment: 7 pages. arXiv admin note: text overlap with arXiv:1107.202
Hydrodynamic and kinetic models for spin-1/2 electron-positron quantum plasmas: Annihilation interaction, helicity conservation, and wave dispersion in magnetized plasmas
We discuss complete theory of spin-1/2 electron-positron quantum plasmas,
when electrons and positrons move with velocities mach smaller than the speed
of light. We derive a set of two fluid quantum hydrodynamic equations
consisting of the continuity, Euler, spin (magnetic moment) evolution equations
for each species. We explicitly include the Coulomb, spin-spin, Darwin and
annihilation interactions. The annihilation interaction is the main topic of
the paper. We consider contribution of the annihilation interaction in the
quantum hydrodynamic equations and in spectrum of waves in magnetized
electron-positron plasmas. We consider propagation of waves parallel and
perpendicular to an external magnetic field. We also consider oblique
propagation of longitudinal waves. We derive set of quantum kinetic equations
for electron-positron plasmas with the Darwin and annihilation interactions. We
apply the kinetic theory for the linear wave behavior in absence of external
fields. We calculate contribution of the Darwin and annihilation interactions
in the Landau damping of the Langmuir waves. We should mention that the
annihilation interaction does not change number of particles in the system. It
does not related to annihilation itself, but it exists as a result of
interaction of an electron-positron pair via conversion of the pair into
virtual photon. A pair of the non-linear Schrodinger equations for
electron-positron plasmas including the Darwin and annihilation interactions.
Existence of conserving helicity in electron-positron quantum plasmas of
spinning particles with the Darwin and annihilation interactions is
demonstrated. We show that annihilation interaction plays an important role in
quantum electron-positron plasmas giving contribution of the same magnitude as
the spin-spin interaction.Comment: 21 pages, 13 figure
First principles derivation of NLS equation for BEC with cubic and quintic nonlinearities at non zero temperature. Dispersion of linear waves
In this work we presented a derivation of the quantum hydrodynamic equations
for neutral bosons. We considered short range interaction between particles.
This interaction consist binary interaction
and three particle interaction
, the last one does not
include binary interaction between particles. From the quantum hydrodynamic
(QHD) equations for Bose-Einstein condensate we derive nonlinear
Schr\"{o}dinger equation. This equation includes the nonlinearities of third
and fifth degree. It is at zero temperature. Explicit form of the constant of
three-particle interaction was taken. First of all, developed method we used
for studying of dispersion of linear waves. Dispersion characteristics of
linear waves were compared for the cases. It were of two-particle interaction
in approximation third order to interaction radius (TOIR) and three-particle
interaction, at zero temperature. We consider influence of temperature on
dispersion of elementary excitations. For this aim we derive a system of QHD
equations at non-zero temperature. Obtained system of equation is an analog of
well-known two-fluid hydrodynamics. Moreover, it is generalization of two-fluid
hydrodynamics equations due to three-particle interaction. Evident expressions
of the velocities of the first and second sound via the concentrations of
superfluid and noncondesate components is calculated.Comment: 14 page
Collective excitations in graphene in magnetic field
Collective excitations in graphene monolayer are studied. Equations
describing collective properties of electrons in graphene are obtained. The
basic ideas of the method of many-particle quantum hydrodynamics are used for
the derivation. As starting point of the derivation we use the Dirac equation
for massless electrons which is usually used for description of electrons in
graphene [D. E. Sheehy and J. Schmalian, Phys. Rev. Lett. 99, 226803 (2007)],
where the Coulomb interaction is taken into account. We study dispersion
properties of collective excitations by means derived here graphene quantum
hydrodynamics equations (GQHD). We consider graphene in the external magnetic
field which directed at an angle to the graphene sample. We do it in a linear
approximation of the GQHD equations. We observe that the magnetic field
directed perpendicular to the graphene plane had no influence on dispersion of
the collective excitations. For the magnetic field directed at an angle to the
graphene we obtain dependence of wave dispersion on system parameters: strength
of magnetic field, wave vector, direction of wave propagation relatively to the
magnetic field.Comment: 7 pages, 3 figure
The quantum hydrodynamic description of quantum gases with different interactions
We describe recent development of quantum hydrodynamics for ultracold Bose
particle studying and consider different kinds of interactions. The method of
derivation of equations describing the evolution of the neutral Bose particle
system at low temperatures is described. Despite the fact that we consider the
neutral particles we account the short-range interaction between particles. We
consider the particles in the Bose-Einstein condensate (BEC) state. This method
is called the method of quantum hydrodynamics, because natural for of the
quantum mechanics rewritten in terms of material fields of observable
quantities in three dimensional space is the set of equations, which look like
the hydrodynamics equations. It can be shown that from the quantum
hydrodynamics equations can be derived macroscopic non-linear Schrodinger
equation. Most famous non-linear Schrodinger equation is the Gross-Pitaevskii
(GP) equation, which contains nonlinearity of the third degree. There are
generalizations of the GP equation. New term appears in the GP equation at
account of the three-particle interaction. This term contains nonlinearity of
the fifth degree. At more detailed account of the two particle interaction we
come to the nonlocal non-linear Schrodinger equation. This equation contains
spatial derivatives of the order parameter in the non-linear terms caused by
the interaction. In this terminology the GP equation corresponds to the first
order by the interaction radius. For the BEC of the neutral particles with
anisotropic long-range dipole-dipole interaction the generalization of the GP
equation was also suggested. Detailed analyses of the applicability conditions
shows that this equation valid for the system of dipoles parallel to each
other, which do not change their direction, and where the dipole-dipole
interaction interferences translational motion of particles.Comment: 37 page
Radiative corrections to the Coulomb law and model of dense quantum plasmas: Dispersion of waves in magnetized quantum plasmas
Two kinds of the quantum electrodynamic radiative corrections to
electromagnetic interaction and their influence on properties of highly dense
quantum plasmas are considered. Linear radiative correction to the Coulomb
interaction are considered. Its contribution in the spectrum of the Langmuir
waves is presented. The second kind of the radiative corrections is related to
nonlinearity of the Maxwell equations for strong electromagnetic field. Its
contribution in spectrum of transverse waves of magnetized plasmas is briefly
discussed. At consideration of the Langmuir wave spectrum we included effect of
different distribution of the spin-up and spin-down electrons revealing in a
shift of the Fermi pressure.Comment: 5 pages, 1 figur
Oblique propagation of longitudinal spin-electron acoustic waves under the influence of the Coulomb exchange interaction and the quantum Bohm potential
Influence of the exchange interaction on the properties of the spin-electron
acoustic waves at the oblique propagation of waves relatively to the external
magnetic field in the magnetically ordered metals is studied. The spectra of
the Langmuir wave and the Trivelpiece-Gould wave are also considered. It is
well-known that there are two branches of spectrum of the spin-electron
acoustic waves in this regime. Change their properties under influence of the
exchange interaction is studied. The quantum Bohm potential is included either.
The exchange interaction and quantum Bohm potential gives opposite
contributions, but they do not compensate each other since they have different
dependence on the wave vector. This competition creates a non-monotonical
behavior of the Trivelpiece-Gould wave spectrum. The concavity changes in the
monotonic spectra of the Langmuir wave and the SEAWs are found.Comment: 8 pages, 8 figure
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