195 research outputs found

    Genetic diversity of Sclerocarya birrea subspecies birrea populations in Burkina Faso detected by RAPDs

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    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 species’ 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

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    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

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    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

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    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)

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    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

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    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

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    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

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    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’ процСссС ускорСния ΠΊΠΈΠ»ΡŒΠ²Π°Ρ‚Π΅Ρ€Π½Ρ‹ΠΌΠΈ Π²ΠΎΠ»Π½Π°ΠΌΠΈ Π²ΠΎΠ·ΠΌΠΎΠΆΠ½Π° гСнСрация свСрхкоротких элСктронных ΠΏΡƒΡ‡ΠΊΠΎΠ² фСмтосСкундной Π΄Π»ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎΡΡ‚ΡŒΡŽ. Для ΠΏΡ€ΠΈΠ»ΠΎΠΆΠ΅Π½ΠΈΠΉ Ρ‚Ρ€Π΅Π±ΡƒΡŽΡ‚ΡΡ элСктронныС ΠΏΡƒΡ‡ΠΊΠΈ с воспроизводимыми ΠΈ ΠΊΠΎΡ‚Ρ€ΠΎΠ»ΠΈΡ€ΡƒΠ΅ΠΌΡ‹ΠΌΠΈ ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€Π°ΠΌΠΈ. ΠžΠΏΡ‚ΠΈΡ‡Π΅ΡΠΊΠ°Ρ инТСкция, ΠΈΡΠΏΠΎΠ»ΡŒΠ·ΡƒΡŽΡ‰Π°Ρ ΡΡ‚Π°Π»ΠΊΠΈΠ²Π°ΡŽΡ‰ΠΈΠ΅ΡΡ Π»Π°Π·Π΅Ρ€Π½Ρ‹Π΅ ΠΈΠΌΠΏΡƒΠ»ΡŒΡΡ‹, обСспСчиваСт Π²Ρ‹ΡΠΎΠΊΡƒΡŽ Π²ΠΎΡΠΏΡ€ΠΎΠΈΠ·Π²ΠΎΠ΄ΠΈΠΌΠΎΡΡ‚ΡŒ ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€ΠΎΠ² ΠΏΡƒΡ‡ΠΊΠΎΠ² ускорСнных элСктронов. ΠœΠΎΠ½ΠΎΡΠ½Π΅Ρ€Π³Π΅Ρ‚ΠΈΡ‡Π΅ΡΠΊΠΈΠ΅ ΠΏΡƒΡ‡ΠΊΠΈ элСктронов с воспроизводимыми ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€Π°ΠΌΠΈ Π±Ρ‹Π»ΠΈ ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½Ρ‹ ΠΏΡ€ΠΈ «самоинТСкции» Π² ΠΊΠΈΠ»ΡŒΠ²Π°Ρ‚Π΅Ρ€Π½ΡƒΡŽ Π²ΠΎΠ»Π½Ρƒ Π² экспСримСнтах, ΠΈΡΠΏΠΎΠ»ΡŒΠ·ΡƒΡŽΡ‰ΠΈΡ… Π² качСствС мишСни ΡΡ‚Ρ€ΡƒΡŽ Π°Π·ΠΎΡ‚Π°. ВзаимодСйствиС элСктронов с ΠΈΠ·Π»ΡƒΡ‡Π΅Π½ΠΈΠ΅ΠΌ Π»Π°Π·Π΅Ρ€Π½ΠΎΠ³ΠΎ ΠΈΠΌΠΏΡƒΠ»ΡŒΡΠ° ΠΏΡ€ΠΈΠ²ΠΎΠ΄ΠΈΡ‚ ΠΊ ΠΏΠΎΠΏΠ΅Ρ€Π΅Ρ‡Π½Ρ‹ΠΌ осцилляциям элСктронного ΠΏΡƒΡ‡ΠΊΠ°. Анализ наблюдаСмой Π² экспСримСнтС зависимости ΠΏΠ΅Ρ€ΠΈΠΎΠ΄Π° осцилляций ΠΎΡ‚ энСргии элСктронов позволяСт Π½Π°ΠΉΡ‚ΠΈ Π΄Π»ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎΡΡ‚ΡŒ элСктронного ΠΏΡƒΡ‡ΠΊΠ°, Ρ€Π°Π²Π½ΡƒΡŽ 1.7 фс.Π’ процСсі прискорСння ΠΊΡ–Π»ΡŒΠ²Π°Ρ‚Π΅Ρ€Π½ΠΈΠΌΠΈ хвилями ΠΌΠΎΠΆΠ»ΠΈΠ²Π° гСнСрація Π½Π°Π΄ΠΊΠΎΡ€ΠΎΡ‚ΠΊΠΈΡ… Π΅Π»Π΅ΠΊΡ‚Ρ€ΠΎΠ½Π½ΠΈΡ… ΠΏΡƒΡ‡ΠΊΡ–Π² фСмтосСкундної тривалості. Для Π΄ΠΎΠ΄Π°Ρ‚ΠΊΡ–Π² ΠΏΠΎΡ‚Ρ€Ρ–Π±Π½Ρ– Π΅Π»Π΅ΠΊΡ‚Ρ€ΠΎΠ½Π½Ρ– ΠΏΡƒΡ‡ΠΊΠΈ Π· Π²Ρ–Π΄Ρ‚Π²ΠΎΡ€ΡŽΡŽΡ‡ΠΈΠΌΠΈ Ρ– ΠΊΠΎΡ‚Ρ€ΠΎΠ»ΡŽΡŽΡ‡ΠΈΠΌΠΈ ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€Π°ΠΌΠΈ. ΠžΠΏΡ‚ΠΈΡ‡Π½Π° інТСкція, Ρ‰ΠΎ використовує Π·Ρ–ΡˆΡ‚ΠΎΠ²Ρ…ΡƒΡŽΡ‡Ρ– Π»Π°Π·Π΅Ρ€Π½Ρ– Ρ–ΠΌΠΏΡƒΠ»ΡŒΡΠΈ, Π·Π°Π±Π΅Π·ΠΏΠ΅Ρ‡ΡƒΡ” високу Π²Ρ–Π΄Ρ‚Π²ΠΎΡ€ΡŽΠ²Π°Π½Ρ–ΡΡ‚ΡŒ ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€Ρ–Π² ΠΏΡƒΡ‡ΠΊΡ–Π² прискорСних Π΅Π»Π΅ΠΊΡ‚Ρ€ΠΎΠ½Ρ–Π². ΠœΠΎΠ½ΠΎΠ΅Π½Π΅Ρ€Π³Π΅Ρ‚ΠΈΡ‡Π½Ρ– ΠΏΡƒΡ‡ΠΊΠΈ Π΅Π»Π΅ΠΊΡ‚Ρ€ΠΎΠ½Ρ–Π² Π· Π²Ρ–Π΄Ρ‚Π²ΠΎΡ€ΡŽΠ²Π°Π½ΠΈΠΌΠΈ ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€Π°ΠΌΠΈ Π±ΡƒΠ»ΠΈ ΠΎΡ‚Ρ€ΠΈΠΌΠ°Π½Ρ– ΠΏΡ€ΠΈ «самоінТСкції» Π² ΠΊΡ–Π»ΡŒΠ²Π°Ρ‚Π΅Ρ€Π½Ρƒ Ρ…Π²ΠΈΠ»ΡŽ Π² СкспСримСнтах, Π² яких Π² якості ΠΌΡ–ΡˆΠ΅Π½Ρ– використовувалася ΡΡ‚Ρ€ΡƒΠΌΡ–Π½ΡŒ Π°Π·ΠΎΡ‚Ρƒ. Взаємодія Π΅Π»Π΅ΠΊΡ‚Ρ€ΠΎΠ½Ρ–Π² Π· Π²ΠΈΠΏΡ€ΠΎΠΌΡ–Π½ΡŽΠ²Π°Π½Π½ΡΠΌ Π»Π°Π·Π΅Ρ€Π½ΠΎΠ³ΠΎ Ρ–ΠΌΠΏΡƒΠ»ΡŒΡΡƒ ΠΏΡ€ΠΈΠ·Π²ΠΎΠ΄ΠΈΡ‚ΡŒ Π΄ΠΎ ΠΏΠΎΠΏΠ΅Ρ€Π΅Ρ‡Π½ΠΈΡ… осциляцій Π΅Π»Π΅ΠΊΡ‚Ρ€ΠΎΠ½Π½ΠΎΠ³ΠΎ ΠΏΡƒΡ‡ΠΊΠ°. Аналіз ΡΠΏΠΎΡΡ‚Π΅Ρ€Ρ–Π³Π°ΡŽΡ‡ΠΎΡ— Π² СкспСримСнті залСТності ΠΏΠ΅Ρ€Ρ–ΠΎΠ΄Ρƒ осциляцій Π²Ρ–Π΄ Π΅Π½Π΅Ρ€Π³Ρ–Ρ— Π΅Π»Π΅ΠΊΡ‚Ρ€ΠΎΠ½Ρ–Π² дозволяє Π·Π½Π°ΠΉΡ‚ΠΈ Ρ‚Ρ€ΠΈΠ²Π°Π»Ρ–ΡΡ‚ΡŒ Π΅Π»Π΅ΠΊΡ‚Ρ€ΠΎΠ½Π½ΠΎΠ³ΠΎ ΠΏΡƒΡ‡ΠΊΠ°, яка Π΄ΠΎΡ€Ρ–Π²Π½ΡŽΡ” 1.7 фс
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