Time-resolved characteristics of deuteron-beam generated by plasma focus discharge.
The plasma focus device discussed herein is a Z-pinch pulsed-plasma arrangement. In this, the plasma is heated and compressed into a cylindrical column, producing a typical density of > 1025 particles/m3 and a temperature of (1-3) × 107 oC. The plasma focus has been widely investigated as a radia...
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doaj-ad4cb5670c67426cb4749cda810f3d022020-11-24T21:48:14ZengPublic Library of Science (PLoS)PLoS ONE1932-62032018-01-01131e018800910.1371/journal.pone.0188009Time-resolved characteristics of deuteron-beam generated by plasma focus discharge.Lian-Kuang LimSeong-Ling YapD A BradleyThe plasma focus device discussed herein is a Z-pinch pulsed-plasma arrangement. In this, the plasma is heated and compressed into a cylindrical column, producing a typical density of > 1025 particles/m3 and a temperature of (1-3) × 107 oC. The plasma focus has been widely investigated as a radiation source, including as ion-beams, electron-beams and as a source of x-ray and neutron production, providing considerable scope for use in a variety of technological situations. Thus said, the nature of the radiation emission depends on the dynamics of the plasma pinch. In this study of the characteristics of deuteron-beam emission, in terms of energy, fluence and angular distribution were analyzed. The 2.7 kJ plasma focus discharge has been made to operate at a pressure of less than 1 mbar rather than at its more conventional operating pressure of a few mbar. Faraday cup were used to determine deuteron-beam energy and deuteron-beam fluence per shot while CR-39 solid-state nuclear track detectors were employed in studying the angular distribution of deuteron emission. Beam energy and deuteron-beam fluence per shot have been found to be pressure dependent. The largest value of average deuteron energy measured for present conditions was found to be (52 ± 7) keV, while the deuteron-beam fluence per shot was of the order of 1015 ions/m2 when operated at a pressure of 0.2 mbar. The deuteron-beam emission is in the forward direction and is observed to be highly anisotropic.http://europepmc.org/articles/PMC5757925?pdf=render |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Lian-Kuang Lim Seong-Ling Yap D A Bradley |
spellingShingle |
Lian-Kuang Lim Seong-Ling Yap D A Bradley Time-resolved characteristics of deuteron-beam generated by plasma focus discharge. PLoS ONE |
author_facet |
Lian-Kuang Lim Seong-Ling Yap D A Bradley |
author_sort |
Lian-Kuang Lim |
title |
Time-resolved characteristics of deuteron-beam generated by plasma focus discharge. |
title_short |
Time-resolved characteristics of deuteron-beam generated by plasma focus discharge. |
title_full |
Time-resolved characteristics of deuteron-beam generated by plasma focus discharge. |
title_fullStr |
Time-resolved characteristics of deuteron-beam generated by plasma focus discharge. |
title_full_unstemmed |
Time-resolved characteristics of deuteron-beam generated by plasma focus discharge. |
title_sort |
time-resolved characteristics of deuteron-beam generated by plasma focus discharge. |
publisher |
Public Library of Science (PLoS) |
series |
PLoS ONE |
issn |
1932-6203 |
publishDate |
2018-01-01 |
description |
The plasma focus device discussed herein is a Z-pinch pulsed-plasma arrangement. In this, the plasma is heated and compressed into a cylindrical column, producing a typical density of > 1025 particles/m3 and a temperature of (1-3) × 107 oC. The plasma focus has been widely investigated as a radiation source, including as ion-beams, electron-beams and as a source of x-ray and neutron production, providing considerable scope for use in a variety of technological situations. Thus said, the nature of the radiation emission depends on the dynamics of the plasma pinch. In this study of the characteristics of deuteron-beam emission, in terms of energy, fluence and angular distribution were analyzed. The 2.7 kJ plasma focus discharge has been made to operate at a pressure of less than 1 mbar rather than at its more conventional operating pressure of a few mbar. Faraday cup were used to determine deuteron-beam energy and deuteron-beam fluence per shot while CR-39 solid-state nuclear track detectors were employed in studying the angular distribution of deuteron emission. Beam energy and deuteron-beam fluence per shot have been found to be pressure dependent. The largest value of average deuteron energy measured for present conditions was found to be (52 ± 7) keV, while the deuteron-beam fluence per shot was of the order of 1015 ions/m2 when operated at a pressure of 0.2 mbar. The deuteron-beam emission is in the forward direction and is observed to be highly anisotropic. |
url |
http://europepmc.org/articles/PMC5757925?pdf=render |
work_keys_str_mv |
AT liankuanglim timeresolvedcharacteristicsofdeuteronbeamgeneratedbyplasmafocusdischarge AT seonglingyap timeresolvedcharacteristicsofdeuteronbeamgeneratedbyplasmafocusdischarge AT dabradley timeresolvedcharacteristicsofdeuteronbeamgeneratedbyplasmafocusdischarge |
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