Electrical shielding box measurement of the negative hydrogen beam from Penning ion gauge ion source

The cold-cathode Penning ion gauge (PIG) type ion source has been used for generation of negative hydrogen (H(-)) ions as the internal ion source of a compact cyclotron. A novel method called electrical shielding box dc beam measurement is described in this paper, and the beam intensity was measured under dc extraction inside an electrical shielding box. The results of the trajectory simulation and dc H(-) beam extraction measurement were presented. The effect of gas flow rate, magnetic field strength, arc current, and extraction voltage were also discussed. In conclusion, the dc H(-) beam current of about 4 mA from the PIG ion source with the puller voltage of 40 kV and arc current of 1.31 A was extrapolated from the measurement at low extraction dc voltages.     

A Low-Energy Gas-Discharge Open-End Ion Source without the External Magnetic Field

The described ion source, as oppose to the well-known Hall-type open-end ion source does not require an external magnetic field. The optimal operating parameters of the ion source (discharge voltage is 140 V, discharge current is 2.5 A, and operating pressure is <3.5 × 10^–4Torr) allow one to obtain an argon ion beam with a current of up to 200 mA over an area with a diameter of up to 120 mm and beam current nonuniformity of <25%. This ion source has a long service life under high-temperature operating conditions.     

Low-energy, high-current, ion source with cold electron emitter

An ion source based on a two-stage discharge with electron injection from a cold emitter is presented. The first stage is the emitter itself, and the second stage provides acceleration of injected electrons for gas ionization and formation of ion flow (<20 eV, 5 A dc). The ion accelerating system is gridless; acceleration is accomplished by an electric field in the discharge plasma within an axially symmetric, diverging, magnetic field. The hollow cathode electron emitter utilizes an arc discharge with cathode spots hidden inside the cathode cavity. Selection of the appropriate emitter material provides a very low erosion rate and long lifetime.     

A long pulse width and high extraction rate arc plasma electron beam source

Based on the principle of vacuum arc discharge under magnetic field, a novel plasma cathode electron- beam source was designed. This device can be used to regulate electron-beam current so as to improve the extrication efficiency of electron beam through regulating the exciting current and thus controlling the density of the plasma electron beam source. Experiment results showed that the arc current change with the magnetic field, to be specific, the stronger the magnetic field was, the smaller the arc current will be, then the density of plasma that penetrated the anode hole to serve as electron beam will be higher. From this experiment, it can be seen that under the condition of 10^?3 Pa air pressure, 100 V arc voltage, 30 A exciting current, we can obtain the electron beam of 40 ms pulse width, and 828 mA current in the extraction rate of 6.1%.     

Surface plasma source with saddle antenna radio frequency plasma generator

A prototype RF H(-) surface plasma source (SPS) with saddle (SA) RF antenna is developed which will provide better power efficiency for high pulsed and average current, higher brightness with longer lifetime and higher reliability. Several versions of new plasma generators with small AlN discharge chambers and different antennas and magnetic field configurations were tested in the plasma source test stand. A prototype SA SPS was installed in the Spallation Neutron Source (SNS) ion source test stand with a larger, normal-sized SNS AlN chamber that achieved unanalyzed peak currents of up to 67 mA with an apparent efficiency up to 1.6 mA∕kW. Control experiments with H(-) beam produced by SNS SPS with internal and external antennas were conducted. A new version of the RF triggering plasma gun has been designed. A saddle antenna SPS with water cooling is fabricated for high duty factor testing.     

A Universal Ion Source with a Cold Cathode

A plasmotron source of positive low-charge ions of metals and gases with a two-stage discharge is described. The emittances of the ion beams of various elements normalized by the longitudinal velocity and extracted from the source are within 0.1 cm mrad, and the equivalent proton currents of ions accelerated by a voltage of 50 kV are 120–380 mA. A cold cathode is used in the source. Metal ions are produced in the regime of the vacuum arc discharge in cathode material vapors.     

A Wide-Aperture Source of Oxygen Ions with a Hollow Cold Cathode and Magnetic Multicast

A gas-discharge source of oxygen ions is described. The source contains an anode and a hollow cold cathode with one extracting grid (extractor) placed at the opposite end to the anode. The hollow cathode has three multicast magnetic systems of permanent polarity. The first system is placed inside the cathode near the anode, the second system is situated outside the cathode opposite to the first one, and the third system is placed below the second one near the extractor surface. Like poles of the first and second magnetic systems are directed towards each other. The second and third systems have poles of similar orientations. Using this source, a beam of oxygen ions with a current density of up to 0.5 mA/cm² and nonuniformity of <5% was obtained across a 200-mm-diameter area at a distance of 120 mm from the face of the ion source. The source offers the following optimum performance characteristics: a discharge current of 0.4–1.2 A, oxygen flow rate of 9–12 cm³/min, and extracting voltage of 400–600 V. No limitations were revealed on the service life of a source operating in optimal modes.     

Increase in the Charge State of the Uranium Ion Beam Generated by the MEVVA Ion Source

The Metal Vapor Vacuum Arc (MEVVA) ion source and its modifications are investigated at the Institute of Theoretical and Experimental Physics (ITEP). In a series of the experiments, the possibility of increasing the charge state of the generated uranium ion beam was revealed. The charge state increases as a result of developing a high-current vapor vacuum arc discharge from the source cathode to an auxiliary anode located in an increasing axial magnetic field. The uranium ion beam with a total current of 150 mA was obtained, U⁷⁺ uranium ions being 10% of the current.     

An Ion Source with an Open-End Small-Sized Anode

A small-sized gas-discharge ion source is described. The source contains a cylindrical hollow cathode made of a ferromagnetic material with longitudinal magnetization of up to 16 mT; a cone-shaped anode and a cathode-reflector in the form of a tube situated in axial symmetry inside the hollow cathode; and an external thermionic cathode. The overall dimensions of the ion source without the thermionic cathode are 45 × 44 mm. The source ensures an argon ion beam current of up to 80 mA at a discharge current and voltage of 1 A and 115 V, respectively, and a pressure of 1.5 × 10⁻² Pa in the chamber. The minimum operating pressure is 0.8 × 10⁻² Pa.__________Translated from Pribory i Tekhnika Eksperimenta, No. 3, 2005, pp. 147–149.Original Russian Text Copyright © 2005 by Stognij, Zavadskaya, Koryakin, Lobko, Yurchenko.     

Generation of Gas Discharge Plasma by an Arc Source with a Cold Hollow Cathode

The results from a study of an arc plasma source with a cold hollow cathode are presented. The source generates plasma with a density of ∼10¹⁰ cm⁻³ in a volume of ∼0.2 m³ at discharge currents of up to 150 A, an arc discharge operating voltage of 30–40 V, and a low pressure of 0.1–1 Pa. The motion of the cathode spot in the crossed electric and magnetic fields inside the hollow cathode and the cathode’s special design make it possible to eliminate almost completely the penetration of the sputtered cathode material into the working vacuum chamber.__________Translated from Pribory i Tekhnika Eksperimenta, No. 3, 2005, pp. 62–66.Original Russian Text Copyright © 2005 by Schanin, Koval, Akhmadeev.     

Development of low-energy and high-current-density ion beam system

A low-energy ion beam system operating at a dc voltage of less than 300 V was developed using an ion source with a multicusp magnetic field. A high-current-density ion beam of 6.9 mA∕cm(2) was successfully extracted at the electrode. The beam extraction characteristics for flat and concave electrodes were compared. In the case of a concave electrode with a designed focal length of 350 mm, it was observed that the beam profile was sharper than that obtained using a flat electrode.     

Microwave ion source for high-current implanter

A long-life, high-current, microwave ion source for an electromagnetic mass separator is described. Ionization takes place due to the 2.45-GHz microwave discharge at a magnetic field intensity which is higher than the electron cyclotron resonance magnetic field. The discharge chamber is a ridged circular waveguide. The discharge region is restricted to a rectangular volume between the ridged electrodes by filling the remaining portions with dielectric. This source operates under low pressure (10(-2)-10(-3) Torr) and with high power efficiency. The incident microwave power is only several hundred watts at maximum output. When PH(3) gas is introduced, the total extracted current is about 40 mA with a 2x40-mm extraction slit. A P(+) ion implantation current of more than 10 mA is obtained by combining the source with a 40-cm radius, 60 degrees deflection magnetic mass separator.     

脉冲真空电弧离子镀发射特性的测量

通过大量工艺实验 ,镀制了改变脉冲真空电弧离子源电源参数 (主回路电压 ,脉冲频率 )、基片高度以及磁场等工艺参数的样品 ,选择了一种合适的膜厚测量仪器进行了膜厚分布测量 ,获得了离子源各种工艺参数对其发射特性影响的曲线     

高能量离子束诊断质谱仪的研制及性能表征

本研究开发了一台应用于高能量离子束诊断的直线式飞行时间质谱仪，实现了其与高能真空弧放电离子源的联用。该仪器加速电压30 kV，飞行腔有效飞行距离1.5 m，通过短脉冲离子门精确截取，ICCD高速相机优化聚焦，仪器分辨率优于90 FWHM，对放电过程中产生的等离子体可实现不同时间的离子成分分析。将该方法用于真空弧放电离子源放电过程中离子成分的检测，放电2 μs时，电离成分以气态离子C⁺、O⁺、C²⁺、O²⁺为主；放电6 μs后，除气体成分外，还可以检测到Fe⁺、Cu⁺及其同位素金属离子峰。该仪器能够给出离子源放电产生离子的种类、价态以及相对含量等信息，可实现整个放电过程产生离子成分信息的准确诊断。     

A new extraction system for the Linac4 H- ion source

As part of the CERN accelerator complex upgrade, a new linear accelerator for H(-) (Linac4) is under construction. The ion source design is based on the non-caesiated DESY RF-driven ion source, with the goal of producing an H(-) beam of 80 mA beam current, 45 keV beam energy, 0.4 ms pulse length, and 2 Hz repetition rate. The source has been successfully commissioned for an extraction voltage of 35 kV, corresponding to the one used at DESY. Increasing the extraction voltage to 45 kV has resulted in frequent high voltage breakdowns in the extraction region caused by evaporating material from the electron dump, triggering a new design of the extraction and electron dumping system. Results of the ion source commissioning at 35 kV are presented as well as simulations of a new pulsed extraction system for beam extraction at 45 kV.     

Gas discharge ion source. I. Duoplasmatron

The effects of the plasma expansion cup on the operation of a duoplasmatron ion source have been investigated by measuring the total ion current and the distributions of the ion energy, mass, and current density. A copper expansion cup did not affect the magnetic field near the anode of the ion source and consequently the ion current density distribution was sharply peaked near the center of the cup. Ion energy distributions were approximately symmetrical about anode potential. The dominant ionic species were D(+) (3) and D(+) at low and high arc currents, respectively. Changes in the electrical potential of the copper cup with respect to the anode produced negligible changes in the above data. A mild steel plasma expansion cup caused the magnetic field to diverge and intercept the cup walls, resulting in ion current density distributions that were flatter and more amenable to focusing than the ones with the copper cup. With the steel cup at anode potential, the ion mass distribution was similar to that from the copper cup; however, the ion energy distribution was asymmetrical about the anode potential with a peak about 10-20 V above anode potential. The total ion current from this mode of operation was about one-third the value from the copper cup. If the steel cup assumed floating potential, about 50 V below anode potential, the total current increased to the level observed from the copper cup and the ion energy distribution was similar to that observed with the copper cup but the current density distribution was much flatter than that of the copper cup. The ion mass distribution was 60%-70% atomic ions over the entire arc current range investigated. Based on these data, a modified plasma expansion cup was designed with tapered steel walls lined with a boron nitride insert. The overall performance of the duoplasmatron ion source with this cup was superior to any of the previous three modes of operation. The improved design uses a molybdenum anode insert which is far superior to copper in regard to erosion over extended operating times. A total beam current of 200 mA was produced at an arc current of 24 A.     

A Compact High-Voltage Power Supply for an Accelerating Installation

A compact high-voltage power supply for an accelerating installation that uses high-frequency (25 kHz) voltage conversion is described. The power supply provides a variable voltage of 5 to 100 kV at a load current of up to 250 A and three independently variable voltages of 0–100 V (100 mA), 0–2000 V (5 mA), and 1–15 kV (50 A), which are required for operating the cold-cathode ion source used in the installation. The output-voltage ripple is <0.05%. The power-supply efficiency is no less than 70%.     

Development of a low-energy and high-current pulsed neutral beam injector with a washer-gun plasma source for high-beta plasma experiments

We have developed a novel and economical neutral-beam injection system by employing a washer-gun plasma source. It provides a low-cost and maintenance-free ion beam, thus eliminating the need for the filaments and water-cooling systems employed conventionally. In our primary experiments, the washer gun produced a source plasma with an electron temperature of approximately 5 eV and an electron density of 5 × 10(17) m(-3), i.e., conditions suitable for ion-beam extraction. The dependence of the extracted beam current on the acceleration voltage is consistent with space-charge current limitation, because the observed current density is almost proportional to the 3∕2 power of the acceleration voltage below approximately 8 kV. By optimizing plasma formation, we successfully achieved beam extraction of up to 40 A at 15 kV and a pulse length in excess of 0.25 ms. Its low-voltage and high-current pulsed-beam properties enable us to apply this high-power neutral beam injection into a high-beta compact torus plasma characterized by a low magnetic field.     

稀土永磁无刷直流电动机电磁场有限元分析

应用ANSYS软件对逆变器工作方式为二相导通星形三相六状态的稀土永磁无刷直流电动机的空载和负载电磁场特性进行了有限元分析。分析结果表明：正在研发的稀土永磁无刷直流电动机可得到近似方波的气隙磁感应强度,从而有效减少力矩脉动,提高电动机出力,电动机结构设计和材料选用合理;电源电压从0～100V变化时,电动机的电磁转矩逐渐增大,但增大率逐渐降低。当电源电压增至72V以后,电动机的电磁转矩增大率降至很小。     

Characteristics of low-energy ion beams extracted from a wire electrode geometry

Beams of argon ions with energies less than 50 eV were extracted from an ion source through a wire electrode extractor geometry. A retarding potential energy analyzer (RPEA) was constructed in order to characterize the extracted ion beams. The single aperture RPEA was used to determine the ion energy distribution function, the mean ion energy and the ion beam energy spread. The multi-cusp hot cathode ion source was capable of producing a low electron temperature gas discharge to form quiescent plasmas from which ion beam energy as low as 5 eV was realized. At 50 V extraction potential and 0.1 A discharge current, the ion beam current density was around 0.37 mA/cm(2) with an energy spread of 3.6 V or 6.5% of the mean ion energy. The maximum ion beam current density extracted from the source was 0.57 mA/cm(2) for a 50 eV ion beam and 1.78 mA/cm(2) for a 100 eV ion beam.