195 research outputs found
Genetic diversity of Sclerocarya birrea subspecies birrea populations in Burkina Faso detected by RAPDs
Sclerocarya birrea, multipurpose plant is characteristic of the Sahel-Sudanian savanna and is widespread in West Africa. Although this species has a high socio-economic importance, its genetic organization was not well characterized in Burkina Faso. In this study, the intra and interpopulation genetic diversity of S. birrea was determined by random amplified polymorphic deoxyribonucleic acid (RAPD) markers. We found a high average of intra population genetic diversity (He = 0.20) among S. birrea populations. The species populations were also characterized by their low genetic differentiation (Gst = 0.24), indicating a significant exchange of genes flow between populations. The whole population was clustered into four groups without reference of site and climatic zone. The Mantel test suggested that genetic distances between populations were not correlated to geographic distances. Our results strongly suggest that the structure and the level of this speciesβ genetics diversity may be due to its mode of dissemination involving ruminants.Key words: Genetic, variation, Sclerocarya birrea subspecies birrea, populations, RAPDs markers, Burkina Faso
Opportunities for TeV Laser Acceleration
A set of ballpark parameters for laser, plasma, and accelerator technologies
that define for electron energies reaching as high as TeV are identified. These
ballpark parameters are carved out from the fundamental scaling laws that
govern laser acceleration, theoretically suggested and experimentally explored
over a wide range in the recent years. In the density regime on the order of
10^{16} cm^{-3}, the appropriate laser technology, we find, matches well with
that of a highly efficient high fluence LD driven Yb ceramic laser. Further,
the collective acceleration technique applies to compactify the beam stoppage
stage by adopting the beam-plasma wave deceleration, which contributes to
significantly enhance the stopping power and energy recovery capability of the
beam. Thus we find the confluence of the needed laser acceleration parameters
dictated by these scaling laws and the emerging laser technology. This may
herald a new technology in the ultrahigh energy frontier.Comment: 16 pages, 2 figures, 1 table, submitted to AIP Conference Proceeding
Coulomb implosion mechanism of negative ion acceleration in laser plasmas
Coulomb implosion mechanism of the negatively charged ion acceleration in
laser plasmas is proposed. When a cluster target is irradiated by an intense
laser pulse and the Coulomb explosion of positively charged ions occurs, the
negative ions are accelerated inward. The maximum energy of negative ions is
several times lower than that of positive ions. The theoretical description and
Particle-in-Cell simulation of the Coulomb implosion mechanism and the evidence
of the negative ion acceleration in the experiments on the high intensity laser
pulse interaction with the cluster targets are presented.Comment: 4 page
Transverse Dynamics and Energy Tuning of Fast Electrons Generated in Sub-Relativistic Intensity Laser Pulse Interaction with Plasmas
The regimes of quasi-mono-energetic electron beam generation were
experimentally studied in the sub-relativistic intensity laser plasma
interaction. The observed electron acceleration regime is unfolded with
two-dimensional-particle-in-cell simulations of laser-wakefield generation in
the self-modulation regime.Comment: 10 pages, 5 figure
Lorentz-Abraham-Dirac vs Landau-Lifshitz radiation friction force in the ultrarelativistic electron interaction with electromagnetic wave (exact solutions)
When the parameters of electron - extreme power laser interaction enter the
regime of dominated radiation reaction, the electron dynamics changes
qualitatively. The adequate theoretical description of this regime becomes
crutially important with the use of the radiation friction force either in the
Lorentz-Abraham-Dirac form, which possess unphysical runaway solutions, or in
the Landau-Lifshitz form, which is a perturbation valid for relatively low
electromagnetic wave amplitude. The goal of the present paper is to find the
limits of the Landau-Lifshitz radiation force applicability in terms of the
electromagnetic wave amplitude and frequency. For this a class of the exact
solutions to the nonlinear problems of charged particle motion in the
time-varying electromagnetic field is used.Comment: 14 pages, 5 figure
Soft X-ray harmonic comb from relativistic electron spikes
We demonstrate a new high-order harmonic generation mechanism reaching the
`water window' spectral region in experiments with multi-terawatt femtosecond
lasers irradiating gas jets. A few hundred harmonic orders are resolved, giving
uJ/sr pulses. Harmonics are collectively emitted by an oscillating electron
spike formed at the joint of the boundaries of a cavity and bow wave created by
a relativistically self-focusing laser in underdense plasma. The spike
sharpness and stability are explained by catastrophe theory. The mechanism is
corroborated by particle-in-cell simulations
Observation of Burst Intensification by Singularity Emitting Radiation generated from relativistic plasma with a high-intensity laser
Coherent x-rays via the Burst Intensification by Singularity Emitting Radiation (BISER) mechanism are generated from relativistic plasma in helium gas target. A broad modulation of the BISER spectrum, which is significantly wider than the harmonic order, is observed and characterized. In particular, we found that the modulation period can be as large as 41 eV
Stability improvement of a laser-accelerated electron beam and the pulse width measurement of the electron beam
Laser wakefield acceleration has the possibility to generate an ultrashort electron beam of the order of femtoseconds or less. In applications of these laser accelerated electron beams, stable and controllable electron beams are necessary. A high stability electron bunch is generated by laser wakefield acceleration with the help of a colliding laser pulse (optical injection). Stable and monoenergetic electron beams have been generated in the self-injection scheme of laser acceleration by using a Nitrogen gas jet target. The electron interaction with the laser field results in transverse oscillations of the electron beam. From the electron oscillation period dependence on the electron energy we find that the electron beam width is equal to 1.7 fs (rms).Π ΠΏΡΠΎΡΠ΅ΡΡΠ΅ ΡΡΠΊΠΎΡΠ΅Π½ΠΈΡ ΠΊΠΈΠ»ΡΠ²Π°ΡΠ΅ΡΠ½ΡΠΌΠΈ Π²ΠΎΠ»Π½Π°ΠΌΠΈ Π²ΠΎΠ·ΠΌΠΎΠΆΠ½Π° Π³Π΅Π½Π΅ΡΠ°ΡΠΈΡ ΡΠ²Π΅ΡΡ
ΠΊΠΎΡΠΎΡΠΊΠΈΡ
ΡΠ»Π΅ΠΊΡΡΠΎΠ½Π½ΡΡ
ΠΏΡΡΠΊΠΎΠ² ΡΠ΅ΠΌΡΠΎΡΠ΅ΠΊΡΠ½Π΄Π½ΠΎΠΉ Π΄Π»ΠΈΡΠ΅Π»ΡΠ½ΠΎΡΡΡΡ. ΠΠ»Ρ ΠΏΡΠΈΠ»ΠΎΠΆΠ΅Π½ΠΈΠΉ ΡΡΠ΅Π±ΡΡΡΡΡ ΡΠ»Π΅ΠΊΡΡΠΎΠ½Π½ΡΠ΅ ΠΏΡΡΠΊΠΈ Ρ Π²ΠΎΡΠΏΡΠΎΠΈΠ·Π²ΠΎΠ΄ΠΈΠΌΡΠΌΠΈ ΠΈ ΠΊΠΎΡΡΠΎΠ»ΠΈΡΡΠ΅ΠΌΡΠΌΠΈ ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΠ°ΠΌΠΈ. ΠΠΏΡΠΈΡΠ΅ΡΠΊΠ°Ρ ΠΈΠ½ΠΆΠ΅ΠΊΡΠΈΡ, ΠΈΡΠΏΠΎΠ»ΡΠ·ΡΡΡΠ°Ρ ΡΡΠ°Π»ΠΊΠΈΠ²Π°ΡΡΠΈΠ΅ΡΡ Π»Π°Π·Π΅ΡΠ½ΡΠ΅ ΠΈΠΌΠΏΡΠ»ΡΡΡ, ΠΎΠ±Π΅ΡΠΏΠ΅ΡΠΈΠ²Π°Π΅Ρ Π²ΡΡΠΎΠΊΡΡ Π²ΠΎΡΠΏΡΠΎΠΈΠ·Π²ΠΎΠ΄ΠΈΠΌΠΎΡΡΡ ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΠΎΠ² ΠΏΡΡΠΊΠΎΠ² ΡΡΠΊΠΎΡΠ΅Π½Π½ΡΡ
ΡΠ»Π΅ΠΊΡΡΠΎΠ½ΠΎΠ². ΠΠΎΠ½ΠΎΡΠ½Π΅ΡΠ³Π΅ΡΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΠΏΡΡΠΊΠΈ ΡΠ»Π΅ΠΊΡΡΠΎΠ½ΠΎΠ² Ρ Π²ΠΎΡΠΏΡΠΎΠΈΠ·Π²ΠΎΠ΄ΠΈΠΌΡΠΌΠΈ ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΠ°ΠΌΠΈ Π±ΡΠ»ΠΈ ΠΏΠΎΠ»ΡΡΠ΅Π½Ρ ΠΏΡΠΈ Β«ΡΠ°ΠΌΠΎΠΈΠ½ΠΆΠ΅ΠΊΡΠΈΠΈΒ» Π² ΠΊΠΈΠ»ΡΠ²Π°ΡΠ΅ΡΠ½ΡΡ Π²ΠΎΠ»Π½Ρ Π² ΡΠΊΡΠΏΠ΅ΡΠΈΠΌΠ΅Π½ΡΠ°Ρ
, ΠΈΡΠΏΠΎΠ»ΡΠ·ΡΡΡΠΈΡ
Π² ΠΊΠ°ΡΠ΅ΡΡΠ²Π΅ ΠΌΠΈΡΠ΅Π½ΠΈ ΡΡΡΡΡ Π°Π·ΠΎΡΠ°. ΠΠ·Π°ΠΈΠΌΠΎΠ΄Π΅ΠΉΡΡΠ²ΠΈΠ΅ ΡΠ»Π΅ΠΊΡΡΠΎΠ½ΠΎΠ² Ρ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΠ΅ΠΌ Π»Π°Π·Π΅ΡΠ½ΠΎΠ³ΠΎ ΠΈΠΌΠΏΡΠ»ΡΡΠ° ΠΏΡΠΈΠ²ΠΎΠ΄ΠΈΡ ΠΊ ΠΏΠΎΠΏΠ΅ΡΠ΅ΡΠ½ΡΠΌ ΠΎΡΡΠΈΠ»Π»ΡΡΠΈΡΠΌ ΡΠ»Π΅ΠΊΡΡΠΎΠ½Π½ΠΎΠ³ΠΎ ΠΏΡΡΠΊΠ°. ΠΠ½Π°Π»ΠΈΠ· Π½Π°Π±Π»ΡΠ΄Π°Π΅ΠΌΠΎΠΉ Π² ΡΠΊΡΠΏΠ΅ΡΠΈΠΌΠ΅Π½ΡΠ΅ Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠΈ ΠΏΠ΅ΡΠΈΠΎΠ΄Π° ΠΎΡΡΠΈΠ»Π»ΡΡΠΈΠΉ ΠΎΡ ΡΠ½Π΅ΡΠ³ΠΈΠΈ ΡΠ»Π΅ΠΊΡΡΠΎΠ½ΠΎΠ² ΠΏΠΎΠ·Π²ΠΎΠ»ΡΠ΅Ρ Π½Π°ΠΉΡΠΈ Π΄Π»ΠΈΡΠ΅Π»ΡΠ½ΠΎΡΡΡ ΡΠ»Π΅ΠΊΡΡΠΎΠ½Π½ΠΎΠ³ΠΎ ΠΏΡΡΠΊΠ°, ΡΠ°Π²Π½ΡΡ 1.7 ΡΡ.Π ΠΏΡΠΎΡΠ΅ΡΡ ΠΏΡΠΈΡΠΊΠΎΡΠ΅Π½Π½Ρ ΠΊΡΠ»ΡΠ²Π°ΡΠ΅ΡΠ½ΠΈΠΌΠΈ Ρ
Π²ΠΈΠ»ΡΠΌΠΈ ΠΌΠΎΠΆΠ»ΠΈΠ²Π° Π³Π΅Π½Π΅ΡΠ°ΡΡΡ Π½Π°Π΄ΠΊΠΎΡΠΎΡΠΊΠΈΡ
Π΅Π»Π΅ΠΊΡΡΠΎΠ½Π½ΠΈΡ
ΠΏΡΡΠΊΡΠ² ΡΠ΅ΠΌΡΠΎΡΠ΅ΠΊΡΠ½Π΄Π½ΠΎΡ ΡΡΠΈΠ²Π°Π»ΠΎΡΡΡ. ΠΠ»Ρ Π΄ΠΎΠ΄Π°ΡΠΊΡΠ² ΠΏΠΎΡΡΡΠ±Π½Ρ Π΅Π»Π΅ΠΊΡΡΠΎΠ½Π½Ρ ΠΏΡΡΠΊΠΈ Π· Π²ΡΠ΄ΡΠ²ΠΎΡΡΡΡΠΈΠΌΠΈ Ρ ΠΊΠΎΡΡΠΎΠ»ΡΡΡΠΈΠΌΠΈ ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΠ°ΠΌΠΈ. ΠΠΏΡΠΈΡΠ½Π° ΡΠ½ΠΆΠ΅ΠΊΡΡΡ, ΡΠΎ Π²ΠΈΠΊΠΎΡΠΈΡΡΠΎΠ²ΡΡ Π·ΡΡΡΠΎΠ²Ρ
ΡΡΡΡ Π»Π°Π·Π΅ΡΠ½Ρ ΡΠΌΠΏΡΠ»ΡΡΠΈ, Π·Π°Π±Π΅Π·ΠΏΠ΅ΡΡΡ Π²ΠΈΡΠΎΠΊΡ Π²ΡΠ΄ΡΠ²ΠΎΡΡΠ²Π°Π½ΡΡΡΡ ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΡΠ² ΠΏΡΡΠΊΡΠ² ΠΏΡΠΈΡΠΊΠΎΡΠ΅Π½ΠΈΡ
Π΅Π»Π΅ΠΊΡΡΠΎΠ½ΡΠ². ΠΠΎΠ½ΠΎΠ΅Π½Π΅ΡΠ³Π΅ΡΠΈΡΠ½Ρ ΠΏΡΡΠΊΠΈ Π΅Π»Π΅ΠΊΡΡΠΎΠ½ΡΠ² Π· Π²ΡΠ΄ΡΠ²ΠΎΡΡΠ²Π°Π½ΠΈΠΌΠΈ ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΠ°ΠΌΠΈ Π±ΡΠ»ΠΈ ΠΎΡΡΠΈΠΌΠ°Π½Ρ ΠΏΡΠΈ Β«ΡΠ°ΠΌΠΎΡΠ½ΠΆΠ΅ΠΊΡΡΡΒ» Π² ΠΊΡΠ»ΡΠ²Π°ΡΠ΅ΡΠ½Ρ Ρ
Π²ΠΈΠ»Ρ Π² Π΅ΠΊΡΠΏΠ΅ΡΠΈΠΌΠ΅Π½ΡΠ°Ρ
, Π² ΡΠΊΠΈΡ
Π² ΡΠΊΠΎΡΡΡ ΠΌΡΡΠ΅Π½Ρ Π²ΠΈΠΊΠΎΡΠΈΡΡΠΎΠ²ΡΠ²Π°Π»Π°ΡΡ ΡΡΡΡΠΌΡΠ½Ρ Π°Π·ΠΎΡΡ. ΠΠ·Π°ΡΠΌΠΎΠ΄ΡΡ Π΅Π»Π΅ΠΊΡΡΠΎΠ½ΡΠ² Π· Π²ΠΈΠΏΡΠΎΠΌΡΠ½ΡΠ²Π°Π½Π½ΡΠΌ Π»Π°Π·Π΅ΡΠ½ΠΎΠ³ΠΎ ΡΠΌΠΏΡΠ»ΡΡΡ ΠΏΡΠΈΠ·Π²ΠΎΠ΄ΠΈΡΡ Π΄ΠΎ ΠΏΠΎΠΏΠ΅ΡΠ΅ΡΠ½ΠΈΡ
ΠΎΡΡΠΈΠ»ΡΡΡΠΉ Π΅Π»Π΅ΠΊΡΡΠΎΠ½Π½ΠΎΠ³ΠΎ ΠΏΡΡΠΊΠ°. ΠΠ½Π°Π»ΡΠ· ΡΠΏΠΎΡΡΠ΅ΡΡΠ³Π°ΡΡΠΎΡ Π² Π΅ΠΊΡΠΏΠ΅ΡΠΈΠΌΠ΅Π½ΡΡ Π·Π°Π»Π΅ΠΆΠ½ΠΎΡΡΡ ΠΏΠ΅ΡΡΠΎΠ΄Ρ ΠΎΡΡΠΈΠ»ΡΡΡΠΉ Π²ΡΠ΄ Π΅Π½Π΅ΡΠ³ΡΡ Π΅Π»Π΅ΠΊΡΡΠΎΠ½ΡΠ² Π΄ΠΎΠ·Π²ΠΎΠ»ΡΡ Π·Π½Π°ΠΉΡΠΈ ΡΡΠΈΠ²Π°Π»ΡΡΡΡ Π΅Π»Π΅ΠΊΡΡΠΎΠ½Π½ΠΎΠ³ΠΎ ΠΏΡΡΠΊΠ°, ΡΠΊΠ° Π΄ΠΎΡΡΠ²Π½ΡΡ 1.7 ΡΡ
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