63 research outputs found
Giga-Gauss scale quasistatic magnetic field generation in an 'escargot' target
A simple setup for the generation of ultra-intense quasistatic magnetic
fields, based on the generation of electron currents with a predefined geometry
in a curved 'escargot' target, is proposed and analysed. Particle-In-Cell
simulations and qualitative estimates show that giga-Gauss scale magnetic
fields may be achieved with existent laser facilities. The described mechanism
of the strong magnetic field generation may be useful in a wide range of
applications, from laboratory astrophysics to magnetized ICF schemes.Comment: Submitted to PRL. arXiv admin note: text overlap with arXiv:1409.524
A plasma solenoid driven by an Orbital Angular Momentum laser beam
A tens of Tesla quasi-static axial magnetic field can be produced in the
interaction of a short intense laser beam carrying an Orbital Angular Momentum
with an underdense plasma. Three-dimensional "Particle In Cell" simulations and
analytical model demonstrate that orbital angular momentum is transfered from a
tightly focused radially polarized laser beam to electrons without any
dissipative effect. A theoretical model describing the balistic interaction of
electrons with laser shows that particles gain angular velocity during their
radial and longitudinal drift in the laser field. The agreement between PIC
simulations and the simplified model identifies routes to increase the
intensity of the solenoidal magnetic field by controlling the orbital angular
momentum and/or the energy of the laser beam
Gain of electron orbital angular momentum in a direct laser acceleration process
Three-dimensional "particle in cell" simulations show that a quasistatic magnetic field can be generated in a plasma irradiated by a linearly polarized Laguerre-Gauss beam with a nonzero orbital angular momentum (OAM). Perturbative analysis of the electron dynamics in the low intensity limit and detailed numerical analysis predict a laser to electrons OAM transfer. Plasma electrons gain angular velocity thanks to the dephasing process induced by the combined action of the ponderomotive force and the laser induced-radial oscillation Similar to the "direct laser acceleration," where Gaussian laser beams transmit part of its axial momentum to electrons, Laguerre-Gaussian beams transfer a part of their orbital angular momentum to electrons through the dephasing process
Landau damping in thin films irradiated by a strong laser field
The rate of linear collisionless damping (Landau damping) in a classical
electron gas confined to a heated ionized thin film is calculated. The general
expression for the imaginary part of the dielectric tensor in terms of the
parameters of the single-particle self-consistent electron potential is
obtained. For the case of a deep rectangular well, it is explicitly calculated
as a function of the electron temperature in the two limiting cases of specular
and diffuse reflection of the electrons from the boundary of the
self-consistent potential. For realistic experimental parameters, the
contribution of Landau damping to the heating of the electron subsystem is
estimated. It is shown that for films with a thickness below about 100 nm and
for moderate laser intensities it may be comparable with or even dominate over
electron-ion collisions and inner ionization.Comment: 15 pages, 2 figure
Melting Point and Lattice Parameter Shifts in Supported Metal Nanoclusters
The dependencies of the melting point and the lattice parameter of supported
metal nanoclusters as functions of clusters height are theoretically
investigated in the framework of the uniform approach. The vacancy mechanism
describing the melting point and the lattice parameter shifts in nanoclusters
with decrease of their size is proposed. It is shown that under the high vacuum
conditions (p<10^-7 torr) the essential role in clusters melting point and
lattice parameter shifts is played by the van der Waals forces of
cluster-substrate interation. The proposed model satisfactorily accounts for
the experimental data.Comment: 6 pages, 3 figures, 1 tabl
Π‘ΡΠ°Π²Π½ΠΈΡΠ΅Π»ΡΠ½ΠΎΠ΅ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠ΅ ΡΠ»Π΅ΠΊΡΡΠΎΠΈΡΠΊΡΠΎΠ²ΡΡ ΠΏΠΎΠΊΡΡΡΠΈΠΉ, ΠΏΠΎΠ»ΡΡΠ΅Π½Π½ΡΡ Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ ΡΠ»Π΅ΠΊΡΡΠΎΠ΄ΠΎΠ² TiCβNiCr ΠΈ TiCβNiCrβEu2O3
The study covers coatings obtained on 40Kh steel substrates by electro-spark deposition (ESD) using TiCβNiCr and TiCβNiCrβ Eu2O3 electrodes. Coatings were deposited by the Alier-Metal 303 unit in argon environment under the normal pressure using direct and opposite polarity. The structure, elemental and phase composition of electrodes and coatings were studied using X-ray phase analysis, scanning electron microscopy, energy dispersive spectroscopy, glow discharge optical emission spectroscopy, and optical profilometry. Mechanical and tribological properties of coatings were determined by nanoindentation and testing according to the Β«pin-diskΒ» scheme including high-temperature conditions in the range of 20β500 Β°C. The tests conducted include abrasive wear tests using the Calowear tester, impact resistance tests using the CemeCon impact tester, and tests for gas and electrochemical corrosion resistance. Test results showed that electrodes contain titanium carbide, nickel-chromium solid solution, and europium oxide in case of a doped sample. Coatings exhibit the same phase composition but solid solution is formed on the iron base. Coatings with the Eu2O3 additive do not differ significantly in structural characteristics, hardness, friction coefficient, and exceed the base coatings in terms of their abrasive resistance, repeated impact resistance, heat and corrosion resistance. There was an increase in impact resistance by 1.2β2.0 times, a decrease in corrosion current by more than 20 times, and an oxidation index by almost 2 times during the transition to doped coatings.ΠΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½Ρ ΠΏΠΎΠΊΡΡΡΠΈΡ, ΠΏΠΎΠ»ΡΡΠ΅Π½Π½ΡΠ΅ Π½Π° ΠΏΠΎΠ΄Π»ΠΎΠΆΠΊΠ°Ρ
ΠΈΠ· ΡΡΠ°Π»ΠΈ 40Π₯ ΠΌΠ΅ΡΠΎΠ΄ΠΎΠΌ ΡΠ»Π΅ΠΊΡΡΠΎΠΈΡΠΊΡΠΎΠ²ΠΎΠ³ΠΎ Π»Π΅Π³ΠΈΡΠΎΠ²Π°Π½ΠΈΡ Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ ΡΠ»Π΅ΠΊΡΡΠΎΠ΄ΠΎΠ² TiCβNiCr ΠΈ TiCβNiCrβEu2O3. ΠΠΎΠΊΡΡΡΠΈΡ Π½Π°Π½ΠΎΡΠΈΠ»ΠΈΡΡ Ρ ΠΏΠΎΠΌΠΎΡΡΡ ΡΡΡΠ°Π½ΠΎΠ²ΠΊΠΈ Β«Alier-Metal 303Β» Π² ΡΡΠ΅Π΄Π΅ Π°ΡΠ³ΠΎΠ½Π° ΠΏΡΠΈ Π½ΠΎΡΠΌΠ°Π»ΡΠ½ΠΎΠΌ Π΄Π°Π²Π»Π΅Π½ΠΈΠΈ Π² ΡΠ΅ΠΆΠΈΠΌΠ΅ ΠΏΡΡΠΌΠΎΠΉ ΠΈ ΠΎΠ±ΡΠ°ΡΠ½ΠΎΠΉ ΠΏΠΎΠ»ΡΡΠ½ΠΎΡΡΠΈ. Π‘ΡΡΡΠΊΡΡΡΠ°, ΡΠ»Π΅ΠΌΠ΅Π½ΡΠ½ΡΠΉ ΠΈ ΡΠ°Π·ΠΎΠ²ΡΠΉ ΡΠΎΡΡΠ°Π²Ρ ΡΠ»Π΅ΠΊΡΡΠΎΠ΄ΠΎΠ² ΠΈ ΠΏΠΎΠΊΡΡΡΠΈΠΉ Π±ΡΠ»ΠΈ ΠΈΠ·ΡΡΠ΅Π½Ρ ΠΏΠΎΡΡΠ΅Π΄ΡΡΠ²ΠΎΠΌ ΡΠ΅Π½ΡΠ³Π΅Π½ΠΎΡΠ°Π·ΠΎΠ²ΠΎΠ³ΠΎ Π°Π½Π°Π»ΠΈΠ·Π°, ΡΠ°ΡΡΡΠΎΠ²ΠΎΠΉ ΡΠ»Π΅ΠΊΡΡΠΎΠ½Π½ΠΎΠΉ ΠΌΠΈΠΊΡΠΎΡΠΊΠΎΠΏΠΈΠΈ, ΡΠ½Π΅ΡΠ³ΠΎΠ΄ΠΈΡΠΏΠ΅ΡΡΠΈΠΎΠ½Π½ΠΎΠΉ ΡΠΏΠ΅ΠΊΡΡΠΎΡΠΊΠΎΠΏΠΈΠΈ, ΠΎΠΏΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΠΌΠΈΡΡΠΈΠΎΠ½Π½ΠΎΠΉ ΡΠΏΠ΅ΠΊΡΡΠΎΡΠΊΠΎΠΏΠΈΠΈ ΡΠ»Π΅ΡΡΠ΅Π³ΠΎ ΡΠ°Π·ΡΡΠ΄Π° ΠΈ ΠΎΠΏΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΏΡΠΎΡΠΈΠ»ΠΎΠΌΠ΅ΡΡΠΈΠΈ. ΠΠ΅Ρ
Π°Π½ΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΠΈ ΡΡΠΈΠ±ΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΡΠ²ΠΎΠΉΡΡΠ²Π° ΠΏΠΎΠΊΡΡΡΠΈΠΉ ΠΎΠΏΡΠ΅Π΄Π΅Π»ΡΠ»ΠΈΡΡ ΠΌΠ΅ΡΠΎΠ΄ΠΎΠΌ Π½Π°Π½ΠΎΠΈΠ½Π΄Π΅Π½ΡΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΠΈ ΠΏΡΡΠ΅ΠΌ ΠΈΡΠΏΡΡΠ°Π½ΠΈΠΉ ΠΏΠΎ ΡΡ
Π΅ΠΌΠ΅ Β«ΡΡΠ΅ΡΠΆΠ΅Π½ΡβΠ΄ΠΈΡΠΊΒ», Π² ΡΠΎΠΌ ΡΠΈΡΠ»Π΅ ΠΏΡΠΈ ΠΏΠΎΠ²ΡΡΠ΅Π½Π½ΡΡ
ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΠ°Ρ
Π² Π΄ΠΈΠ°ΠΏΠ°Π·ΠΎΠ½Π΅ 20β500 Β°Π‘. ΠΡΠΎΠ²Π΅Π΄Π΅Π½Ρ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ Π½Π° Π°Π±ΡΠ°Π·ΠΈΠ²Π½ΡΠΉ ΠΈΠ·Π½ΠΎΡ Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ ΠΏΡΠΈΠ±ΠΎΡΠ° Β«Calowear-testerΒ», ΡΡΠΎΠΉΠΊΠΎΡΡΡ ΠΊ Π΄ΠΈΠ½Π°ΠΌΠΈΡΠ΅ΡΠΊΠΈΠΌ Π²ΠΎΠ·Π΄Π΅ΠΉΡΡΠ²ΠΈΡΠΌ Ρ ΠΏΠΎΠΌΠΎΡΡΡ ΡΡΡΠ°Π½ΠΎΠ²ΠΊΠΈ Β«CemeCon impact-testerΒ» ΠΈ ΡΡΠΎΠΉΠΊΠΎΡΡΡ ΠΊ Π³Π°Π·ΠΎΠ²ΠΎΠΉ ΠΈ ΡΠ»Π΅ΠΊΡΡΠΎΡ
ΠΈΠΌΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΊΠΎΡΡΠΎΠ·ΠΈΠΈ. ΠΠΎΠ»ΡΡΠ΅Π½Π½ΡΠ΅ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ ΠΏΠΎΠΊΠ°Π·Π°Π»ΠΈ, ΡΡΠΎ ΡΠ»Π΅ΠΊΡΡΠΎΠ΄Ρ ΡΠΎΠ΄Π΅ΡΠΆΠ°Ρ ΠΊΠ°ΡΠ±ΠΈΠ΄ ΡΠΈΡΠ°Π½Π°, ΡΠ²Π΅ΡΠ΄ΡΠΉ ΡΠ°ΡΡΠ²ΠΎΡ Π½ΠΈΠΊΠ΅Π»Ρ Π² Ρ
ΡΠΎΠΌΠ΅ ΠΈ ΠΎΠΊΡΠΈΠ΄ Π΅Π²ΡΠΎΠΏΠΈΡ Π² ΡΠ»ΡΡΠ°Π΅ Π΄ΠΎΠΏΠΈΡΠΎΠ²Π°Π½Π½ΠΎΠ³ΠΎ ΠΎΠ±ΡΠ°Π·ΡΠ°. ΠΠΎΠΊΡΡΡΠΈΡ ΡΠ°ΠΊΠΆΠ΅ Π²ΠΊΠ»ΡΡΠ°Π»ΠΈ Π΄Π°Π½Π½ΡΠ΅ ΡΠ°Π·Ρ, ΠΎΠ΄Π½Π°ΠΊΠΎ ΡΠ²Π΅ΡΠ΄ΡΠΉ ΡΠ°ΡΡΠ²ΠΎΡ ΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π»ΡΡ Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ ΠΆΠ΅Π»Π΅Π·Π°. ΠΠΎΠΊΡΡΡΠΈΡ Ρ Π΄ΠΎΠ±Π°Π²ΠΊΠΎΠΉ Eu2O3 ΠΏΠΎ ΡΡΡΡΠΊΡΡΡΠ½ΡΠΌ Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΠΊΠ°ΠΌ, ΡΠ²Π΅ΡΠ΄ΠΎΡΡΠΈ, ΠΊΠΎΡΡΡΠΈΡΠΈΠ΅Π½ΡΡ ΡΡΠ΅Π½ΠΈΡ ΡΡΡΠ΅ΡΡΠ²Π΅Π½- Π½ΠΎ Π½Π΅ ΠΎΡΠ»ΠΈΡΠ°Π»ΠΈΡΡ, Π° ΠΏΠΎ ΡΡΠΎΠΉΠΊΠΎΡΡΠΈ ΠΊ Π°Π±ΡΠ°Π·ΠΈΠ²Π½ΠΎΠΌΡ ΠΈΠ·Π½ΠΎΡΡ ΠΈ ΠΊ ΡΠΈΠΊΠ»ΠΈΡΠ΅ΡΠΊΠΈΠΌ ΡΠ΄Π°ΡΠ½ΡΠΌ Π½Π°Π³ΡΡΠ·ΠΊΠ°ΠΌ, ΠΆΠ°ΡΠΎ- ΠΈ ΠΊΠΎΡΡΠΎΠ·ΠΈΠΎΠ½Π½ΠΎΠΉ ΡΡΠΎΠΉΠΊΠΎΡΡΠΈ ΠΏΡΠ΅Π²ΠΎΡΡ
ΠΎΠ΄ΠΈΠ»ΠΈ Π±Π°Π·ΠΎΠ²ΡΠ΅ ΠΏΠΎΠΊΡΡΡΠΈΡ. ΠΠ°Π±Π»ΡΠ΄Π°Π»ΠΈΡΡ ΡΠ²Π΅Π»ΠΈΡΠ΅Π½ΠΈΠ΅ ΡΡΠΎΠΉΠΊΠΎΡΡΠΈ ΠΊ ΡΠ΄Π°ΡΠ½ΡΠΌ Π½Π°Π³ΡΡΠ·ΠΊΠ°ΠΌ Π² 1,2β2,0 ΡΠ°Π·Π°, ΠΏΠΎΠ½ΠΈΠΆΠ΅Π½ΠΈΠ΅ ΡΠΎΠΊΠ° ΠΊΠΎΡΡΠΎΠ·ΠΈΠΈ Π±ΠΎΠ»Π΅Π΅ ΡΠ΅ΠΌ Π² 20 ΡΠ°Π· ΠΈ ΡΠΌΠ΅Π½ΡΡΠ΅Π½ΠΈΠ΅ ΠΏΠΎΠΊΠ°Π·Π°ΡΠ΅Π»Ρ ΠΎΠΊΠΈΡΠ»Π΅Π½ΠΈΡ ΠΏΠΎΡΡΠΈ Π² 2 ΡΠ°Π·Π° ΠΏΡΠΈ ΠΏΠ΅ΡΠ΅Ρ
ΠΎΠ΄Π΅ ΠΊ Π΄ΠΎΠΏΠΈΡΠΎΠ²Π°Π½Π½ΡΠΌ ΠΏΠΎΠΊΡΡΡΠΈΡΠΌ
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