75 research outputs found

    Carbon Multicharged Ion Generation From Laser-Spark Ion Source

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    Multicharged carbon ions are generated by using a laser-assisted spark-discharge ion source. A Q-switched Nd:YAG laser pulse (1064 nm, 7 ns, ≤ 4.5 × 109 W/cm2) focused onto the surface of a glassy carbon target results in its ablation. The spark-discharge (∼1.2 J energy, ∼1 µs duration) is initiated along the direction of the plume propagation between the target surface and a grounded mesh that is parallel to the target surface. Ions emitted from the laser-spark plasma are detected by their time-of-flight using a Faraday cup. The ion energy-to-charge ratio is analyzed by a three-mesh retarding field analyzer. In one set of experiments, the laser plasma is generated by target ablation using a 50 mJ laser pulse. In another set of experiments, ∼1.2 J spark-discharge energy is coupled to the expanding plasma to increase the plasma density and temperature that results in the generation of carbon multicharged ions up to C6+. A delay-generator is used to control the time delay between the laser pulse and the thyratron trigger. Ion generation from a laser pulse when a high DC voltage is applied to the target is compared to that when a spark-discharge with an equivalent pulsed voltage is applied to the target. The laser-coupled spark-discharge (7 kV peak voltage, 810 A peak current) increases the maximum detected ion charge state from C4+ to C6+, accompanied by an increase in the ion yield by a factor of ∼6 compared to applying 7.0 kV DC voltage to the target

    Reconstructing the global topology of the universe from the cosmic microwave background

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    If the universe is multiply-connected and sufficiently small, then the last scattering surface wraps around the universe and intersects itself. Each circle of intersection appears as two distinct circles on the microwave sky. The present article shows how to use the matched circles to explicitly reconstruct the global topology of space.Comment: 6 pages, 2 figures, IOP format. To be published in the proceedings of the Cleveland Cosmology and Topology Workshop 17-19 Oct 1997. Submitted to Class. Quant. Gra

    Space-charge sheath with ions accelerated into the plasma

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    International audienceThe conventional model of near-cathode space-charge sheath with ions entering the sheath from the quasi-neutral plasma may be not applicable to discharges burning in cathode vapor, e.g., vacuum arcs, where ionization of emitted atoms may occur inside the sheath with some of the produced ions returning to the cathode and others moving into the plasma. In this connection, a simple model is considered of a sheath formed by electrons and positive ions injected into the sheath with a very low velocity and moving from the sheath into the plasma. It is shown that such sheath is possible provided that the sheath voltage is equal to or exceeds approximately 1.256kT e /e. This limitation is due to the space charge in the sheath and is in this sense analogous to the limitation of ion current in a vacuum diode expressed by the Child-Langmuir law. The ions leave a sheath and enter the plasma with a velocity equal to or exceeding approximately 1.585u B

    Plasma-Randschicht mit aktiver Oberfläche (Teil 1)

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    Expansion Model of the Neutral Component in Vacuum Arc Spot Plasmas

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    IMPACT AND RESISTIVE HEAT SOURCES OF CATHODE SPOTS IN ARC DISCHARGES

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    Space Charge Sheaths with Electron Emission

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    Plasma-Randschicht mit aktiver Oberfläche (Teil 2)

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    Properties of ideal fermion systems

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