Characterization of intense ion beam energy density and beam induced pressure on the target with acoustic diagnostics

2013 ◽  
Vol 84 (8) ◽  
pp. 083304 ◽  
Author(s):  
A. I. Pushkarev ◽  
Yu. I. Isakova ◽  
Xiao Yu ◽  
I. P. Khailov
2014 ◽  
Vol 32 (2) ◽  
pp. 311-319 ◽  
Author(s):  
A.I. Pushkarev ◽  
Yu.I. Isakova ◽  
I.P. Khaylov

AbstractThis paper presents the results of a statistical and correlation analysis of the energy and energy density of an ion beam formed by a self-magnetically insulated diode with an explosive emission cathode. The experiments were carried out with the TEMP-4M accelerator operating in double-pulse mode: plasma formation occurs during the first pulse (negative polarity, 300–500 ns, 100–150 kV), and ion extraction and acceleration during the second pulse (positive polarity, 120 ns, 250–300 kV). Various arrangements of diodes have been investigated: strip focusing and planar diodes, a conical focusing diode and a spiral diode. The total ion beam energy was measured using both a calorimeter and an infrared camera and the beam energy density was measured by the thermal imaging and acoustic diagnostics. The correlation analysis showed that ion current density is only weakly dependent on the accelerating voltage and other output parameters of the accelerator, with the coefficient of determination <0.3. At the same time, in this paper, we have identified that the total energy of the beam and the energy density is strongly dependant on the accelerator output parameters, since the coefficient of determination >0.9. The mechanism governing stabilization of the beam energy density from shot to shot was discovered and attributed to formation of the neutral component in ion beam as being due to charge exchange between accelerated ions and neutral molecules from a neutral layer near the anode surface. Implementation using a self-magnetically insulated diode with an explosive-emission cathode, having an operational lifetime of up to 106 shots, has promising prospects for various technological applications.


2014 ◽  
Vol 47 (4) ◽  
pp. 1252-1260 ◽  
Author(s):  
Bertrand Clair ◽  
Aziza Ikni ◽  
Wenjing Li ◽  
Philippe Scouflaire ◽  
Vincent Quemener ◽  
...  

Non-photochemical laser-induced nucleation (NPLIN) has been a growing field of study since 1996, and more than 40 compounds including organics, inorganics and proteins have now been probed under various conditions (solvents, laser types, laser beamsetc.). The potential advantages of using this technique are significant, in particular polymorphic control. To realize these benefits, the objective is a carefully designed experimental setup and highly controlled parameters, for example temperature and energy density, in order to reduce the uncertainty regarding the origin of nucleation. In this paper, a new experimental setup designed to study NPLIN is reported. After a full technical description of the present setup, the different functionalities of this device will be illustrated through results on glycine. Glycine crystals obtained through NPLIN nucleate at the meniscus and exhibit different morphologies. The nucleation efficiency, as a function of the supersaturation of the solution used and the laser beam energy density, has also been established for a large number of samples, with all other parameters held constant.


1991 ◽  
Vol 243 ◽  
Author(s):  
Chen C. Li ◽  
Seshu B. Desu

AbstractPbTiO3 and PbZrO3 thin films were successfully fabricated from oxide multilayers by employing ion-assisted deposition process (IAD). Excellent control of the film thickness and composition were achieved by using the multilayer deposition technique. A (001)-oriented phase was found in the PbTiO3 films at 550°C with 300 and 600eV Ar+ ion bombardment. Very fine equiaxial grain size of 0.2μm was seen in the IAD deposited PbTiO3 films, which is independent of the Ar+ ion beam energy. The optical properties of the PbTiO3 films were studied for different energies of Ar+ ion beam and for various post-deposition annealing temperatures. PbTiO3 films with packing density of near unity (≅0.99) were obtained at temperatures as low as 600°C.


MRS Bulletin ◽  
1996 ◽  
Vol 21 (8) ◽  
pp. 58-62 ◽  
Author(s):  
Harold A. Davis ◽  
Gennady E. Remnev ◽  
Regan W. Stinnett ◽  
Kiyoshi Yatsui

Over the past decade, researchers in Japan, Russia, and the United States have been investigating the application of intense-pulsed-ion-beam (IPIB) technology (which has roots in inertial confinement fusion programs) to the surface treatment and coating of materials. The short range (0.1–10 μm) and high-energy density (1–50 J/cm2) of these short-pulsed (t ≥ 1 μs) beams (with ion currents I = 5–50 kA, and energies E = 100–1,000 keV) make them ideal flash-heat sources to rapidly vaporize or melt the near-surface layer of targets similar to the more familiar pulsed laser deposition (PLD) or laser surface treatment. The vaporized material can form coatings on substrates, and surface melting followed by rapid cooling (109 K/s) can form amorphous layers, dissolve precipitates, and form nonequilibrium microstructures.An advantage of this approach over laser processing is that these beams deliver 0.1–10 KJ per pulse to targets at expected overall electrical efficiencies (i.e., the ratio of extracted ion-beam energy to the total energy consumed in generating the beam) of 15–40% (compared to < 1% for the excimer lasers often used for similar applications). Consequently IPIB hardware can be compact and require relatively low capital investment. This opens the promise of environmentally conscious, low-cost, high-throughput manufacturing. Further, efficient beam transport to the target and excellent coupling of incident ion energy to targets are achieved, as opposed to lasers that may have limited coupling to reflective materials or produce reflecting plasmas at high incident fluence. The ion range is adjustable through selection of the ion species and kinetic energy, and the beam energy density can be tailored through control of the beam footprint at the target to melt (1–10 J/cm2) or to vaporize (10–50 J/cm2) the target surface. Beam pulse durations are short (≥ 1 μs) to minimize thermal conduction. Some disadvantages of IPIB processing over laser processing include the need to form and propagate the beams in vacuum, and the need for shielding of x-rays produced by relatively low-level electron current present in IPIB accelerators. Also these beams cannot be as tightly focused onto targets as lasers, making them unsuitable for applications requiring treatment on small spatial scales.


2015 ◽  
Vol 1084 ◽  
pp. 30-33
Author(s):  
Polina A. Beloglazova ◽  
Ivan P. Chernov ◽  
Yuriy P. Cherdantsev ◽  
Natalia Pushilina

We have researched the influence of the carbon pulse ion beam on samples of technical titanium VT1-0. The beam energy was 200 kV; the pulse duration, 80 ns; the energy density, 1.92 J/cm2. It was established that the 1.8 µm deep modified layer with high hardness and low rate of hydrogen sorption in the bulk of material was formed during the exposure to the carbon pulse ion beam.


2021 ◽  
pp. 71-78
Author(s):  
Sergei Kurashkin ◽  
Vadim Tynchenko ◽  
Yuriy Seregin ◽  
Aleksandr Murygin ◽  
Aleksey Bocharov

Sign in / Sign up

Export Citation Format

Share Document