Two Modes of Transportation of a High Current Ion Beam with Ballistic Focusing; Energy Fluxes and Radiation Effects (EFRE-2020 online)
| Parent link: | Energy Fluxes and Radiation Effects (EFRE-2020 online).— 2020.— [P. 671-674] |
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| Zusammenfassung: | Title screen Ion sources are used to modify surface layers of different materials and manufactured items. The minimization of radiation damage of treated surfaces sets the trend to decrease the ion beam energy (<1.5 keV). The dynamic ion beam compensation and the ion beam plasma generation should be considered to control the transport of the metallic low-energy ion beam with ballistic focusing. The ion beam transport with ballistic focusing in the equipotential drift space is studied with numerical simulation by the 2.5D axial symmetric version of the KARAT electromagnetic PiC code. It is shown that the collector current changes to the pulsed mode when the injected ion energy W<; Wc , where Wc is critical energy that depends on the gas concentration and the injected ion current. The pulsed mode is the result of the virtual anode (VA) formation and its compensation by secondary electrons. In hemispherical drift space with curvature radius of 7.5 cm, the critical energy Wc=2 keV when the transported ion current Ib=1 A and the gas concentration ng=1013 cm-3 . The oscillation frequency of the collector current depends on energy, the system geometry and the gas concentration. The oscillating mode of the collector current when decreasing the energy (W<; Wc ) of the transported ions is a result of the decreased role of secondary electrons in compensating the ion beam space charge. This leads to alternating formations: the VA formation when compensation of the space charge of the beam ions compensated. Plasma in the beam transport area is formed. A critical factor that impacts the ion beam transport mode is the electron heating under the increased plasma instability. All these processes are considered in the proposed PiC simulation. The time required to the ion-beam plasma formation and the period of the collector current pulses decrease as the transported ion energy W and the gas concentration increase. Режим доступа: по договору с организацией-держателем ресурса |
| Sprache: | Englisch |
| Veröffentlicht: |
2020
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| Online-Zugang: | https://doi.org/10.1109/EFRE47760.2020.9241905 |
| Format: | Elektronisch Buchkapitel |
| KOHA link: | https://koha.lib.tpu.ru/cgi-bin/koha/opac-detail.pl?biblionumber=663053 |
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| 200 | 1 | |a Two Modes of Transportation of a High Current Ion Beam with Ballistic Focusing |f T. V. Koval, V. Tarakanov | |
| 203 | |a Text |c electronic | ||
| 300 | |a Title screen | ||
| 320 | |a [References: p. 674 (21 tit.)] | ||
| 330 | |a Ion sources are used to modify surface layers of different materials and manufactured items. The minimization of radiation damage of treated surfaces sets the trend to decrease the ion beam energy (<1.5 keV). The dynamic ion beam compensation and the ion beam plasma generation should be considered to control the transport of the metallic low-energy ion beam with ballistic focusing. The ion beam transport with ballistic focusing in the equipotential drift space is studied with numerical simulation by the 2.5D axial symmetric version of the KARAT electromagnetic PiC code. It is shown that the collector current changes to the pulsed mode when the injected ion energy W<; Wc , where Wc is critical energy that depends on the gas concentration and the injected ion current. The pulsed mode is the result of the virtual anode (VA) formation and its compensation by secondary electrons. In hemispherical drift space with curvature radius of 7.5 cm, the critical energy Wc=2 keV when the transported ion current Ib=1 A and the gas concentration ng=1013 cm-3 . The oscillation frequency of the collector current depends on energy, the system geometry and the gas concentration. The oscillating mode of the collector current when decreasing the energy (W<; Wc ) of the transported ions is a result of the decreased role of secondary electrons in compensating the ion beam space charge. This leads to alternating formations: the VA formation when compensation of the space charge of the beam ions compensated. Plasma in the beam transport area is formed. A critical factor that impacts the ion beam transport mode is the electron heating under the increased plasma instability. All these processes are considered in the proposed PiC simulation. The time required to the ion-beam plasma formation and the period of the collector current pulses decrease as the transported ion energy W and the gas concentration increase. | ||
| 333 | |a Режим доступа: по договору с организацией-держателем ресурса | ||
| 463 | 0 | |0 (RuTPU)RU\TPU\network\34152 |t Energy Fluxes and Radiation Effects (EFRE-2020 online) |o proceedings of 7th International Congress, September 14-26, 2020, Tomsk, Russia |f National Research Tomsk Polytechnic University (TPU) ; Institute of Electrical and Electronics Engineers (IEEE) ; ed. N. A. Ratakhin |v [P. 671-674] |d 2020 | |
| 610 | 1 | |a электронный ресурс | |
| 610 | 1 | |a труды учёных ТПУ | |
| 610 | 1 | |a plasma | |
| 610 | 1 | |a virtual anode | |
| 610 | 1 | |a ballistic focusing | |
| 610 | 1 | |a ion beam transport | |
| 610 | 1 | |a плазма | |
| 610 | 1 | |a виртуальный анод | |
| 610 | 1 | |a перенос | |
| 610 | 1 | |a пучки | |
| 610 | 1 | |a баллистическая фокусировка | |
| 700 | 1 | |a Koval |b T. V. |c mathematician, physicist |c Professor of Tomsk Polytechnic University, Doctor of physical and mathematical sciences |f 1953- |g Tamara Vasilievna |3 (RuTPU)RU\TPU\pers\34227 | |
| 701 | 1 | |a Tarakanov |b V. |g Vladimir | |
| 712 | 0 | 2 | |a Национальный исследовательский Томский политехнический университет |b Инженерная школа информационных технологий и робототехники |c 2017- |x TPU |7 ca |8 rus |9 28330 |
| 801 | 2 | |a RU |b 63413507 |c 20210203 |g RCR | |
| 856 | 4 | |u https://doi.org/10.1109/EFRE47760.2020.9241905 | |
| 942 | |c CF | ||