833 research outputs found
Thermofield-Bosonization on Compact Space
We develop the construction of fermionic fields in terms of bosonic ones to
describe free and interaction models in the circle, using thermofielddynamics.
The description in the case of finite temperature is developed for both normal
modes and zero modes. The treatment extends the thermofield-bosonization for
periodic space
Spiral Patterns and Shocks in Low-compressibility Accretion Disks around Collapsed Objects: Two-dimensional SPH Modeling
In recent years contrasting results have been found regarding the onset of spiral structures and shock fronts in accretion disks around compact objects. Indeed, according to some authors, spiral structures and shock fronts do not develop if an adiabatic index γ > 1.16 is adopted. On the contrary, other authors obtain well-developed spiral patterns and shocks adopting γ = 1.2. In this paper, by using a smoothed particle hydrodynamics (SPH) code, we show that clear spiral patterns and strong radial shocks come out even in very low compressibility (γ = 1.3 > 1.16) accretion disk models in close binaries if the primary is a massive black hole (MBH) with a mass 30-60 times larger than the secondary, whatever the geometrical and dynamical conditions at the inner Lagrangian point, L1, may be, independent of sonic or subsonic injection flow boundary conditions. Indeed, the rationale of this work is that in close binary systems in which the primary is a MBH and the secondary is a low-mass star, we have enough initial energy and angular momentum at the inner Lagrangian point, L1, and a wide and deep enough primary potential well to favor the development of well-defined spiral structures, and eventually spiral shocks, independent of the gas compressibility. According to our results the presence of a MBH triggers the development of spiral structures and spiral shock fronts in the accretion disk both at its outer edge and in the disk bulk, because of the high particle concentration and the strong collisions induced by the strongly accelerated stream particles with the high initial angular momentum at L1
Higher-Derivative Two-Dimensional Massive Fermion Theories
We consider the canonical quantization of a generalized two-dimensional
massive fermion theory containing higher odd-order derivatives. The
requirements of Lorentz invariance, hermiticity of the Hamiltonian and absence
of tachyon excitations suffice to fix the mass term, which contains a
derivative coupling. We show that the basic quantum excitations of a
higher-derivative theory of order 2N+1 consist of a physical usual massive
fermion, quantized with positive metric, plus 2N unphysical massless fermions,
quantized with opposite metrics. The positive metric Hilbert subspace, which is
isomorphic to the space of states of a massive free fermion theory, is selected
by a subsidiary-like condition. Employing the standard bosonization scheme, the
equivalent boson theory is derived. The results obtained are used as a
guideline to discuss the solution of a theory including a current-current
interaction.Comment: 23 pages, Late
Origin of long-period Alfv{\'e}n waves in the solar wind
We suggest that the observed long-period Alfv{\'e}n waves in the solar wind
may be generated in the solar interior due to the pulsation of the Sun in the
fundamental radial mode. The period of this pulsation is about 1 hour. The
pulsation causes a periodical variation of density and large-scale magnetic
field, this affecting the Alfv{\'e}n speed in the solar interior. Consequently
the Alfv{\'e}n waves with the half frequency of pulsation (i.e. with the double
period) can be parametrically amplified in the interior below the convection
zone due to the recently suggested swing wave-wave interaction. Therefore the
amplified Alfv{\'e}n waves have periods of several hours. The waves can
propagate upwards through the convection zone to the solar atmosphere and cause
the observed long-period Alfv{\'e}n oscillations in the solar wind.Comment: 5 pages, 2 figures, accepted in MNRAS Letter
Parity properties of an advection-dominated solar \alpha^2\Om-dynamo
We have developed a high-precision code which solves the kinematic dynamo
problem both for given rotation law and meridional flow in the case of a low
eddy diffusivity of the order of cm/s known from the sunspot
decay. All our models work with an \alf-effect which is positive (negative) in
the northern (southern) hemisphere. It is concentrated in radial layers located
either at the top or at the bottom of the convection zone. We have also
considered an \alf-effect uniformly distributed in all the convection zone. In
the present paper the main attention is focused on i) the parity of the
solution, ii) the form of the butterfly diagram and iii) the phase relation of
the resulting field components. If the helioseismologically derived internal
solar rotation law is considered, a model without meridional flow of high
magnetic Reynolds number (corresponding to low eddy diffusivity) fails in all
the three issues in comparison with the observations. However, a meridional
flow with equatorial drift at the bottom of the convection zone of few meters
by second can indeed enforce the equatorward migration of the toroidal magnetic
field belts similar to the observed butterfly diagram but, the solution has
only a dipolar parity if the (positive) \alf-effect is located at the base of
the convection zone rather than at the top. We can, therefore, confirm the main
results of a similar study by Dikpati & Gilman (2001).Comment: 9 pages, 16 figures, to appear on Astronomy and Astrophysic
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