413 research outputs found
Quantum oscillations of rectified dc voltage as a function of magnetic field in an "almost" symmetric superconducting ring
Periodic quantum oscillations of a rectified dc voltage Vdc(B) vs the
perpendicular magnetic field B were measured near the critical temperature Tc
in a single superconducting aluminum almost symmetric ring (without specially
created circular asymmetry) biased by alternating current with a zero dc
component. With varying bias current and temperature, these Vdc(B) oscillations
behave like the Vdc(B) oscillations observed in a circular-asymmetric ring but
are of smaller amplitude. The Fourier spectra of the Vdc(B) functions exhibit a
fundamental frequency, corresponding to the ring area, and its higher
harmonics. Unexpectedly, satellite frequencies depending on the structure
geometry and external parameters were found next to the fundamental frequency
and around its higher harmonics.Comment: author english version, 2 pages, 3 figires, Proc. of the XXXIV
Conference on Low-Temperature Physics "NT-34" (Russia, 2006
Dynamics of ring dark solitons in Bose-Einstein condensates and nonlinear optics
Quasiparticle approach to dynamics of dark solitons is applied to the case of
ring solitons. It is shown that the energy conservation law provides the
effective equations of motion of ring dark solitons for general form of the
nonlinear term in the generalized nonlinear Schroedinger or Gross-Pitaevskii
equation. Analytical theory is illustrated by examples of dynamics of ring
solitons in light beams propagating through a photorefractive medium and in
non-uniform condensates confined in axially symmetric traps. Analytical results
agree very well with the results of our numerical simulations.Comment: 10 pages, 4 figure
Initiation of Ignition of Highly Fuel Particles in The Flow of High Temperature Medium
An approximate analytical solution of ignition of the fuel porous particles has been brought. The impact of thermal radiation on the characteristics and conditions of the ignition has been considered. The verification of the solution has been obtained by comparing the calculated characteristics (delay time of ignition and the ignition temperature) with similar values obtained using the previously derived formulas
Instabilities in the two-dimensional cubic nonlinear Schrodinger equation
The two-dimensional cubic nonlinear Schrodinger equation (NLS) can be used as
a model of phenomena in physical systems ranging from waves on deep water to
pulses in optical fibers. In this paper, we establish that every
one-dimensional traveling wave solution of NLS with trivial phase is unstable
with respect to some infinitesimal perturbation with two-dimensional structure.
If the coefficients of the linear dispersion terms have the same sign then the
only unstable perturbations have transverse wavelength longer than a
well-defined cut-off. If the coefficients of the linear dispersion terms have
opposite signs, then there is no such cut-off and as the wavelength decreases,
the maximum growth rate approaches a well-defined limit.Comment: 4 pages, 4 figure
Terms and Characteristics of Homogeneous Ignition of Coal-Water Particles Coated with a Water Film
The problem of coal-water fuel ignition of particles in a high-temperature heating has been solved numericallyin the framework of a two-layer model of "coal-water". The basic characteristics of the integrated ignition has been shown. The influence of the vaporization process of the water film on the ignition conditions has been shown
Localized structures of electromagnetic waves in hot electron-positronplasmas
The dynamics of relativistically strong electromagnetic (EM) wave propagation
in hot electron-positron plasma is investigated. The possibility of finding
localized stationary structures of EM waves is explored. It is shown that under
certain conditions the EM wave forms a stable localized soliton-like structures
where plasma is completely expelled from the region of EM field location.Comment: 14 pages, LaTeX, 1 figure can be obtained upon request through email
to [email protected]
Disorder driven quantum critical behavior in CuGeO3 doped with magnetic impurity
For the CuGeO3 doped with 1% of Fe the quantum critical behavior in a wide
temperature range 1-40 K is reported. The critical exponents for susceptibility
along different crystallographic axes are determined: a=0.34 (B//a and B//c)
and a=0.31 (B//b). New effect of the frequency dependence of the critical
exponent is discussed.Comment: Submitted to SCES0
Current-sheet formation in incompressible electron magnetohydrodynamics
The nonlinear dynamics of axisymmetric, as well as helical, frozen-in vortex
structures is investigated by the Hamiltonian method in the framework of ideal
incompressible electron magnetohydrodynamics. For description of current-sheet
formation from a smooth initial magnetic field, local and nonlocal nonlinear
approximations are introduced and partially analyzed that are generalizations
of the previously known exactly solvable local model neglecting electron
inertia. Finally, estimations are made that predict finite-time singularity
formation for a class of hydrodynamic models intermediate between that local
model and the Eulerian hydrodynamics.Comment: REVTEX4, 5 pages, no figures. Introduction rewritten, new material
and references adde
Theory and computation of covariant Lyapunov vectors
Lyapunov exponents are well-known characteristic numbers that describe growth
rates of perturbations applied to a trajectory of a dynamical system in
different state space directions. Covariant (or characteristic) Lyapunov
vectors indicate these directions. Though the concept of these vectors has been
known for a long time, they became practically computable only recently due to
algorithms suggested by Ginelli et al. [Phys. Rev. Lett. 99, 2007, 130601] and
by Wolfe and Samelson [Tellus 59A, 2007, 355]. In view of the great interest in
covariant Lyapunov vectors and their wide range of potential applications, in
this article we summarize the available information related to Lyapunov vectors
and provide a detailed explanation of both the theoretical basics and numerical
algorithms. We introduce the notion of adjoint covariant Lyapunov vectors. The
angles between these vectors and the original covariant vectors are
norm-independent and can be considered as characteristic numbers. Moreover, we
present and study in detail an improved approach for computing covariant
Lyapunov vectors. Also we describe, how one can test for hyperbolicity of
chaotic dynamics without explicitly computing covariant vectors.Comment: 21 pages, 5 figure
Heavy ion beam probe design study for TCABR
The Heavy Ion Beam Probe (HIBP) diagnostic is known as a unique tool for the direct plasma electric potential measurements. It gives also information on plasma density, temperature and current profile. The method is based on the injection of single charged ion beam into the plasma and the registration of the double charged particles born due to collisions with the plasma electrons. The area of the ionization in plasma is the sample volume of the plasma potential measurements. The position and the size of the sample volume are determined by the calculation of the trajectories of the probing particles. Three schemes have been analysed: Cs⁺, Tl⁺ ion and neutral injection for TCABR parameters: B0 = 1.5 T, Ipl = 135 kA. The calculations show that ion probing allows getting radial profiles of TCABR plasma parameters with the injection angle fast scan system. In all cases of ion beam injection we must use a curved beam line for ion beam transportation from last steering plates towards upper port. The primary ion beam injector must be situated out of high magnetic field area and its length is about 1.5m. The energy range (less than 100 keV for Cs⁺, or Tl⁺) allows using compact and cheap ion gun equipmenСистема зондування плазми пучком важких іонів відома як унікальний інструмент для прямих вимірювань потенціалу плазми. Вона також дозволяє одержувати інформацію про густину плазми, температуру і профіль току. Метод заснований на інжекції пучка однозарядних іонів у плазму та реєстрації двозарядних часток, утворених у результаті зіткнень з електронами плазми. Область іонізації у плазмі визначає елементарний об’єм, у якому здійснюється вимірювання потенціалу плазми. Положення і розмір елементарного об’єму визначається за допомогою розрахунків траєкторій зондуючих часток. Проаналізовано три варіанти: інжекція іонів Cs⁺, Tl⁺ та нейтральних атомів для параметрів TCABR: B0 = 1.5 T, Ipl = 135 кA. Розрахунки показують можливість одержання профілів параметрів плазми TCABR за допомогою системи швидкого сканування по кутам інжекції іонного пучка. У всіх випадках інжекції іонного пучка необхідно застосування вигнутого іонопроводу для транспортування іонного пучка від вихідних відхиляючих пластин до порту токамака. Інжектор первинного іонного пучка повинен бути розташований поза областю сильного магнітного поля , а його довжина буде біля 1,5 м. Енергія іонного пучка (біля 100 кеВ для Cs⁺ або Tl⁺) дозволяє застосувати компактний и дешевий іонний інжектор.Система зондирования плазмы пучком тяжелых ионов известна как уникальный инструмент для прямых измерений потенциала плазмы. Она так же позволяет получать информацию о плотности плазмы, температуре и профиле тока. Метод основан на инжекции пучка однозарядных ионов в плазму и регистрации двухзарядных частиц, образующихся в результате столкновений с электронами плазмы. Область ионизации в плазме определяет элементарный объем, в котором происходит измерение потенциала плазмы. Положение и размер элементарного объема определяются с помощью расчета траекторий зондирующих частиц. Проанализировано три варианта: инжекция ионов Cs⁺, Tl⁺ и нейтральных атомов для параметров TCABR: B0 = 1.5 T, Ipl = 135 kA. Расчеты показывают возможность получения профилей параметров плазмы TCABR с помощью системы быстрого сканирования по углу инжекции ионного пучка. Во всех случаях инжекции ионного пучка необходимо использование изогнутого ионопровода для транспортировки ионного пучка от выходных отклоняющих пластин до порта токамака. Инжектор первичного ионного пучка должен быть расположен вне области сильного магнитного поля , а его длина составит около 1,5 м. Энергия ионного пучка (около 100 кэВ для Cs⁺ или Tl⁺) позволяет использовать компактный и дешевый ионный инжектор
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