共查询到20条相似文献,搜索用时 31 毫秒
1.
2.
We describe a new technique to measure the UV/visible absorption spectrum of the ablated material during the laser pulse.
The technique utilizes the continuum emission from one laser produced plasma as a light source to measure the absorption properties
of a second laser produced plasma which is formed on a semi-transparent target with an array of 40 μm holes. A 6 ns, 1064
nm laser was used to ablate a Ag target and the plasma absorption was measured in the range 450–625 nm for a laser fluence
of 1 J cm−2. The total absorption cross-section is (0.5–1.5)×10−17 cm2 in the range 450–540 nm. By comparing the measured absorption with a calculation using the plasma spectroscopy code FLYCHK
it can be concluded that, in the wavelength region examined here, the absorption is mainly due to bound-bound transitions. 相似文献
3.
Pogorelsky I. V. Polyanskiy M. N. Babzien M. Yakimenko V. Dover N. P. Palmer C. A. J. Najmudin Z. Schreiber J. Shkolnikov P. Dudnikova G. 《Laser Physics》2011,21(7):1288-1294
A picosecond CO2 laser was used successfully in a number of experiments exploring advanced methods of particle acceleration [1]. Proton acceleration
from gas-jet plasma exemplifies another advantage of employing the increase in laser wavelength from the optical to the mid-IR
region. Recent theoretical- and experimental-studies of ion acceleration from laser-generated plasma point to better ways
to control the ion beam’s energy when plasma approaches the critical density. Studying this regime with solid-state lasers
is problematic due to the dearth of plasma sources at the critical electron density ∼1021 cm−3, corresponding to laser wavelength λ = 1 μm. CO2 laser offers a solution. The CO2 laser’s 10 μm wavelength shifts the critical plasma density to 1019 cm−3, a value attainable with gas jets. Capitalizing on this approach, we focused a circular polarized 1-TW CO2 laser beam onto a hydrogen gas jet and observed a monoenergetic proton beam in the 1–2 MeV range. Simultaneously, we optically
probed the laser/plasma interaction region with visible light, revealing holes bored by radiation pressure, as well as quasi-stationary
soliton-like plasma formations. Our findings from 2D PIC simulations agree with experimental results and aid in their interpretation. 相似文献
4.
This is a study of target destruction and the dynamics of surface plasma formation during the interaction of quasicontinuous
laser radiation (λ = 1.06 μm, q = 1–7 MW/cm2, τ ∼ 1.5 msec) with D16T duraluminum and bismuth in nitrogen atmospheres at pressures p = 1–20 atm. High speed photography and spectroscopy of the erosion plasma flare are used to determine the onset time for
vaporization of the target, as well as the times of appearance of erosion and nitrogen plasmas for different gas pressures
and laser energy fluxes q. The emergence of the plasma front from the vapor zone into the surrounding nitrogen is detected experimentally and the properties
of the nitrogen plasma are studied. 相似文献
5.
An electron-emitting source generating a low-energy beam measuring 1–3 cm in diameter, with current up to 300 A, pulse duration
within 50–200 μs, and pulse repetition frequency up to 10 Hz is investigated in a gas-filled diode with a mesh plasma cathode
at the accelerating voltage up to 25 kV. The beam is transported in a longitudinal pulsed magnetic field to a distance of
up to 30 cm towards the region of its interaction with a solid. For the current densities up to 100 A/cm2, it provides the power density as high as 10–100 J/cm2 sufficient to melt surfaces of metals, alloys, and composite (metalloceramic) materials within one or a few pulses. This
makes this beam useful for modification of material surfaces and articles made thereof. Using the methods of optical, scanning
and diffraction electron microscopy, by building micro-and nanohardness profiles, and via identification of the treated surface
roughness, the phase composition and the substructure state of the materials subjected to pulsed low-energy e-beam of sub-millimeter
durations are investigated. Formation of submicro-and nanocrystalline multi-phase structure is observed, which ensures a multiple
increase in physico-mechanical and tribological characteristics of the treated material.
__________
Translated from Izvestiya Vysshikh Uchebnykh Zavedenii, Fizika, No. 5, pp. 60–70, May, 2008. 相似文献
6.
A. Caruso N. N. Demchenko V. V. Demchenko S. G. Garanin V. V. Gavrilov A. Yu. Gol'tsov A. I. Gromov S. Yu. Gus'kov Yu. S. Kas'yanov G. A. Kirillov V. N. Kondrashov N. G. Koval'skii I. G. Lebo Yu. A. Merkul'ev V. V. Nikishin V. B. Rozanov A. A. Rupasov R. V. Stepanov C. Strangio S. A. Sukharev V. F. Tishkin G. A. Vergunova N. V. Zmitrenko 《Journal of Russian Laser Research》2000,21(4):335-369
The paper is devoted to recent results concerning investigation of physical processes occurring in a “laser greenhouse” target.
Results of experimental and theoretical studies of laser-pulse interaction with a low-density absorber of the target, namely,
with a porous substance having density close to the plasma critical density, are presented. On the basis of a vast cycle of
experiments carried out in a number of laboratories, it is shown that the absorption of the laser radiation in porous media,
including those with a density exceeding the critical one by at least a factor of 4 to 6, has a bulk nature and is distributed
over the target depth. In particular, the laser-radiation absorption region in a porous substance with density 10−3–10−2 g/cm3 is extended into the target 400–100 μm, respectively. The coefficient of absorption of laser radiation with intensity 1014–1015 W/cm2 in porous substances, including those of the supercritical density, is 70–90%. Experiments have not shown enhanced (compared
to a solid-state target) radiation intensity associated with a possible development of parametric instabilities in an extended
laser plasma of low-density porous media, as well as noticeable contribution of fast electrons to the energy balance and their
effect on the energy transfer. In this paper, theoretical models are developed explaining features of the laser-radiation
absorption and energy transfer in porous media. These models are based on the phenomenon of laser-radiation interaction with
solid components of a porous substance and plasma production inside pores and cells of the medium. The efficiency of energy
conversion in the vicinity of the ignition threshold for the laser-greenhouse target is investigated in the case of an absorber
having the above properties. Numerical calculations have shown that a thermonuclear-gain coefficient of 1 to 2 (with respect
to the energy absorbed) is attained for a laser-radiation energy of 100 kJ.
Translated from Preprint No. 58 of the P. N. Lebedev Physical Institute, Moscow (1999). 相似文献
7.
P. M. Schanin N. N. Koval V. S. Tolkachev V. I. Gushenets 《Russian Physics Journal》2000,43(5):427-431
This paper considers the physical processes associated with the extraction of electrons from the gas discharge plasma in plasma
emitters where the emission boundary is stabilized with a fine grid. The ways of improving the uniformity of the emission
current density distribution are discussed. Accelerators designed on the basis of plasma emitters are capable of producing
pulsed beams of current 10–103 A, current density 0.1–1.0 A/cm2, pulse duration 10−7–10−3 s, and cross-sectional area up to 104 cm2.
Institute of High-Current Electronics, Siberian Division of the Russian Academy of Sciences. Translated from Izvestiya Vysshikh
Uchebnykh Zavedenii, Fizika, No. 5, pp. 92–96, April, 2000. 相似文献
8.
The Raman spectrum of polycrystalline α-naphthylamine was recorded in the region 100–4000 cm−1. Polarisation measurements were made in CS2 and CHCl3 solutions. The infrared spectrum was recorded in nujol mull in the region 200–4000 cm−1. The resolution was better than 2 cm−1 and the accuracy of the measurements was within ± 2 cm−1 for all the spectra. Vibrational assignments have been proposed for the observed frequencies. Out of the 54 normal modes
of vibrations, 51 modes could be observed experimentally. 相似文献
9.
A. É. Bugrov S. Yu. Gus’kov V. B. Rozanov I. N. Burdonskii V. V. Gavrilov A. Yu. Gol’tsov E. V. Zhuzhukalo N. G. Koval’skii V. N. Kondrashov M. I. Pergament V. M. Petryakov S. D. Tsoi 《Journal of Experimental and Theoretical Physics》1999,88(3):441-448
We have experimentally investigated the interaction of high-power neodymium laser pulses in the intensity range 1013–1014 W/cm2 with flat low-density (0.5–10 mg/cm3) agar-agar targets under conditions of interest for problems of inertial nuclear fusion. Optical and x-ray methods with high
temporal and spatial resolution were used to examine the dependence of absorption and scattering of the incident beam on the
initial mean density and thickness of the irradiated samples. We show that when a porous target is irradiated, a bulk absorption
layer of high-temperature plasma is produced inside the target whose dimensions are determined by the initial density of the
material. The time dependence and spectral composition of the harmonics 2ω
0 and 3ω
0/2 observed in the plasma-scattered radiation are measured. A theoretical model is developed that describes the interaction
of high-power laser pulses with a porous medium. Predictions of the model, based on the hypothesis of two stages of homogenization
of the target material—a fast stage (0.1–0.3 ns) and a slow stage (1–3 ns), are in good agreement with the experimental data.
Zh. éksp. Teor. Fiz. 115, 805–818 (March 1999) 相似文献
10.
The dynamics of near-surface plasma formation and the formation of an erosion plasma flame was investigated for quasi-continuous
laser radiation (λ=1.06 μm, q=0.1–10 MW/cm2, τ∼1.5 msec) acting on bismuth targets in air. The absence of low-threshold plasma formation at q<2 MW/cm2 was established and explained. Instabilities in the plasma formation were revealed and the range of laser radiation power
densities (2≤q≤4 MW/cm2) at which these instabilities take place was determined. At q≥5.4 MW/cm2, brightening of the flame was noted. The dependence of the luminescence temperature of the flame on the laser radiation power
density q was determined.
Institute of Molecular and Atomic Physics, National Academy of Sciences of Belarus, 70, F. Skorina Ave., Minsk, 220072, Belarus.
Translated from Zhurnal Prikladnoi Spektroskopii, Vol. 65, No. 1, pp. 126–133, January–February, 1998. 相似文献
11.
R. M. Vlasova N. V. Drichko O. O. Drozdova R. N. Lyubovskaya 《Physics of the Solid State》1997,39(8):1165-1170
The reflection spectra and optical conductivity spectra of the new organic conductor ϰ-(ET)2[Hg(SCN)2Cl] with a metal-insulator transition in the spectral regions 700–5500 and 9000–40 000 cm−1 have been studied in polarized light at 300 K. A comparisonis made between the spectra obtained and the corresponding spectra
of related isostructural conductors based on the ET molecule, and also the properties of the crystal structure of the investigated
compounds. An electronic transition between the ET molecules of the dimer (ET)
2
+
in the spectral region 700–5500 cm−1 has been identified, as have the features of the electronic-vibrational structure arising as a consequence of the interaction
of this transition with the completely symmetric intramolecular vibrations of the ET molecule. It is found that the conductor
with the stronger dimer interaction between the ET molecules has the higher the transition temperature.
Fiz. Tverd. Tela (St. Petersburg) 39, 1313–1319 (August 1997) 相似文献
12.
A sequential three-dimensional (3D) particle-in-cell simulation code PICPSI-3D with a user friendly graphical user interface
(GUI) has been developed and used to study the interaction of plasma with ultrahigh intensity laser radiation. A case study
of laser–plasma-based electron acceleration has been carried out to assess the performance of this code. Simulations have
been performed for a Gaussian laser beam of peak intensity 5 × 1019 W/cm2 propagating through an underdense plasma of uniform density 1 × 1019 cm − 3, and for a Gaussian laser beam of peak intensity 1.5 × 1019 W/cm2 propagating through an underdense plasma of uniform density 3.5 × 1019 cm − 3. The electron energy spectrum has been evaluated at different time-steps during the propagation of the laser beam. When the
plasma density is 1 × 1019 cm − 3, simulations show that the electron energy spectrum forms a monoenergetic peak at ~14 MeV, with an energy spread of ±7 MeV.
On the other hand, when the plasma density is 3.5 × 1019 cm − 3, simulations show that the electron energy spectrum forms a monoenergetic peak at ~23 MeV, with an energy spread of ±7.5 MeV. 相似文献
13.
A. N. Murashkevich A. S. Lavitskaya T. I. Barannikova I. M. Zharskii 《Journal of Applied Spectroscopy》2008,75(5):730-734
The composites xTiO2-(1−x)SiO2 (x = 0.1, 0.5, 0.9) were obtained by coprecipitation from solutions of alkoxides: tetraethoxysilane (TEOS) and titanium tetraisopropoxide
(TIPT). Intermolecular interaction of the components of the composite is apparent in the IR absorption spectra in the 928–952
cm−1 region, and is connected with bending vibrations of the Si-O-Ti bond.
Translated from Zhurnal Prikladnoi Spektroskopii, Vol. 75, No. 5, pp. 724–728, September–October, 2008. 相似文献
14.
I. P. Chernov S. V. Ivanova M. Kh. Krening N. Koval’ V. V. Larionov A. M. Lider N. S. Pushilina E. N. Stepanova O. M. Stepanova Yu. P. Cherdantsev 《Technical Physics》2012,57(3):392-398
A pulsed action of an electron beam on a Zr-1% Nb zirconium alloy is studied. Alloy samples are irradiated by three 50-μs
pulses at an energy density of 15–25 J/cm2, a power of (3–6) × 104 W/cm2, a current density of 10–50 A/cm2, and an electron energy of 18 keV. This method of processing is found to modify the surface layer of the alloy without changing
the structure-phase state of its volume. This surface modification increases the hydrogen saturation resistance of the alloy. 相似文献
15.
V. P. Rotshtein Yu. F. Ivanov A. B. Markov D. I. Proskurovskii K. V. Oskomov V. V. Uglov S. N. Dub Y. Pauleau I. A. Shulepov 《Russian Physics Journal》2005,48(12):1221-1228
The surface topography, chemical composition, microstructure, nanohardness, and tribological characteristics of a Cu (film,
512 nm)-stainless steel 316 (substrate) system subjected to pulsed melting by a low-energy (20–30 keV), high-current electron
beam (2–3 μs, 2–10 J/cm2) were investigated. The film was deposited by sputtering a Cu target in the plasma of a microwave discharge in argon. To
prevent local exfoliation of the film due to cratering, the substrate was multiply pre-irradiated with 8–10 J/cm2. On single irradiation, the bulk of the film survived, and a diffusion layer containing the film and substrate components
was formed at the interface. The thickness of this layer was 120–170 nm irrespective of the energy density. The diffusion
layer consisted of subgrains of γ-Fe solid solution and nanosized particles of copper. In the surface layer of thickness 0.5–1 μm, which included the copper
film quenched from melt and the diffusion layer, the nanohardness and the wear resistance nonmonotonicly varied with energy
density, reaching, respectively, a maximum and a minimum in the range 4.3–6.3 J/cm2. As the number of pulsed melting cycles was increased to five in the same energy density range, there occurred mixing of
the film-substrate system and a surface layer of thickness ∼2 μm was formed which contained ∼20 at. % copper. Displacement
of the excess copper during crystallization resulted in the formation of two-phase nanocrystal interlayers separating the
γ-phase grains.
__________
Translated from Izvestiya Vysshikh Uchebnykh Zavedenii, Fizika, No. 12, pp. 6–13, December, 2005. 相似文献
16.
L. Y. Min'ko A. N. Chumakov A. N. Loparev G. I. Bakanovich V. B. Avramenko 《Journal of Applied Spectroscopy》1998,65(2):273-280
It is established that, in the case of laser action on materials in large illuminated spots in atmospheric-pressure air for
a laser radiation power density q≤2 MW/cm2 (λ=1.315 μm), an evaporative regime with plane scattering of the laser-produced erosion plasma is realized while, for q≈5–17
MW/cm2, the plasma front is transferred to the air, leading to plasma screening of the target and shaping of a subsonic radiation
wave in the air. As the duration of the laser pulses increases (τ∼160 μsec), in spite of the large illuminated spots (S∼150
cm2) the evaporative regime of the laser action with plane plasma scattering goes over into a regime with jet outlow and formation
of a quasistationary shock wave.
Deceased.
Institute of Molecular and Atomic Physics, National Academy of Sciences of Belarus, 70, F. Skorina Ave., Minsk, 220072, Belarus.
Translated from Zhurnal Prikladnoi Spektroskopii, Vol. 65, No. 2, pp. 261–268, March–April, 1998. 相似文献
17.
A. Ya. Faenov S. A. Pikuz A. G. Zidkov I. Yu. Skobelev P. S. Komarov O. V. Chefonov S. V. Gasilov A. V. Ovchinnikov 《JETP Letters》2010,92(6):375-378
The characteristics of X rays of a laser plasma generated in the interaction of a femtosecond pulse with solid targets in
an air atmosphere have been investigated. It has been shown that the mechanism for the generation of X rays in the interaction
of short intense laser pulses with solid targets in a gas atmosphere is attributed to the generation of fast electrons in
the region of the filamentation of a laser pulse. It has been proven experimentally that under such conditions, the solid
target irradiated by laser radiation of even a low density of about 1015 W/cm2 very efficiently emits ∼10-keV photons. It has been shown theoretically that the maximum energy of accelerated electrons
can reach ɛmax ∼ 100–200 keV under these conditions. This means that the proposed method can provide characteristic radiation with the energy
of photons much higher than 10 keV. 相似文献
18.
Experimental diagnostic methods based on the measurement of the reflectance of a plasma are considered. The application of
Fourier interferometry for measuring the dynamics of variation of the amplitude and phase of the complex reflectance of the
Au plasma for various delay times in intervals shorter than 1 ps relative to the pumping laser pulse with a femtosecond time
resolution is described in detail in the intensity range ∼1013–1014 W/cm2. The variation of the complex refractive index of the heated Au target for a pump pulse intensity of ∼1012–1013 W/cm2 is analyzed on the basis of experimental data using the Fresnel formulas. 相似文献
19.
Grafted natural rubber-based polymer electrolytes: ATR-FTIR and conductivity studies 总被引:2,自引:0,他引:2
Attenuated total reflectance–Fourier transformed infrared spectroscopy measurement is employed to study the interactions between
the components of 30% methyl-grafted natural rubber (MG30), lithium trifluromethanesulfonate (LiCF3SO3 or LiTF), and propylene carbonate (PC). Vibrational spectra data of LiTF reveals that the νs(SO3) at 1,045 cm−1, δs(CF3) at 777 cm−1, and C=O stretching mode at 1,728 cm−1 for MG30 have shifted to lower wave numbers in MG30–LiTF complexes indicating that complexation has occurred between MG30
and LiTF. The solvation of lithium ion is manifested in Li+ ← O=C interaction as shown by the downshifting and upshifting of C=O mode at 1,788 to 1,775 cm−1 and νas(SO3) at 1,250 to 1258 cm−1, respectively, in LiTF–PC electrolytes. There is no experimental evidence of the interaction between MG30 and PC. Competition
between MG30 and PC on associating with lithium ion is studied, and the studies show that the interaction between MG30–LiTF
is stronger than that of the PC–LiTF in plasticized polymer–salt complexes. The effect of PC on the ionic conductivity of
the MG30–LiTF system is explained in terms of the polymer, plasticizer, and salt interactions. The temperature dependence
of conductivity of the polymer films obeys the Vogel–Tamman–Fulcher relation. Values of conductivity and activation energy
of the MG30-based polymer electrolyte systems are presented and discussed. 相似文献
20.
Silicon crystals after implantation of erbium ions with energies in the range 0.8–2.0 MeV and doses in the range 1×1012–1×1014 cm−2 have been studied by two-and three-crystal x-ray diffraction. Three types of two-crystal reflection curves are observed.
They correspond to different structural states of the implanted layers. At moderate doses (1×1012–1×1013 cm−2) a positive strain is observed, due to the formation of secondary radiation defects of interstitial type. An increase of
the implantation dose is accompanied by the formation of an amorphous layer separating the bulk layer and a thin monocrystalline
surface layer. At an implantation dose of 1×1014 cm−2 the monocrystalline surface layer is completely amorphized. Parameters of the implantation layers are determined. A model
of the transformation of structural damage is discussed.
Fiz. Tverd. Tela (St. Petersburg) 39, 853–857 (May 1997) 相似文献