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Investigation of the time interval of plasma generation for a high repetition rate laser ion source
To apply a laser ion source that generates a high-intensity pulsed beam to high-dose applications, such as ion implantation, a high repetition rate operation with a short pulse interval is required. However, when the pulse interval is shortened, there is a concern that a plasma, which is different f...
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Published in: | Review of scientific instruments 2020-03, Vol.91 (3), p.033305-033305 |
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creator | Kashiwagi, H. Yamada, K. |
description | To apply a laser ion source that generates a high-intensity pulsed beam to high-dose applications, such as ion implantation, a high repetition rate operation with a short pulse interval is required. However, when the pulse interval is shortened, there is a concern that a plasma, which is different from a single pulse plasma generation, may be formed due to the interaction between the preceding and following pulses. We investigated the time interval in which plasma pulses are generated without pulse-to-pulse interaction using a laser ion source with two lasers. In the experiment, a graphite target was irradiated by two laser beams (1064-nm wavelengths) with the same pulse widths (5.4 ns) and energies (15 mJ, 30 mJ, and 45 mJ) at different time intervals ranging from 1000 μs to 0 µs, and the time integrated value corresponding to the total charge amount was calculated from the measured time-of-flight signal of the generated carbon ion current. It was observed that the total charge did not change when the time interval was as low as approximately 100 µs, and the total charge rapidly decreased when the time interval was below approximately 100 µs. Thus, it was determined that the interaction occurs within a time interval of approximately 100 µs. |
doi_str_mv | 10.1063/1.5130999 |
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However, when the pulse interval is shortened, there is a concern that a plasma, which is different from a single pulse plasma generation, may be formed due to the interaction between the preceding and following pulses. We investigated the time interval in which plasma pulses are generated without pulse-to-pulse interaction using a laser ion source with two lasers. In the experiment, a graphite target was irradiated by two laser beams (1064-nm wavelengths) with the same pulse widths (5.4 ns) and energies (15 mJ, 30 mJ, and 45 mJ) at different time intervals ranging from 1000 μs to 0 µs, and the time integrated value corresponding to the total charge amount was calculated from the measured time-of-flight signal of the generated carbon ion current. It was observed that the total charge did not change when the time interval was as low as approximately 100 µs, and the total charge rapidly decreased when the time interval was below approximately 100 µs. 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However, when the pulse interval is shortened, there is a concern that a plasma, which is different from a single pulse plasma generation, may be formed due to the interaction between the preceding and following pulses. We investigated the time interval in which plasma pulses are generated without pulse-to-pulse interaction using a laser ion source with two lasers. In the experiment, a graphite target was irradiated by two laser beams (1064-nm wavelengths) with the same pulse widths (5.4 ns) and energies (15 mJ, 30 mJ, and 45 mJ) at different time intervals ranging from 1000 μs to 0 µs, and the time integrated value corresponding to the total charge amount was calculated from the measured time-of-flight signal of the generated carbon ion current. It was observed that the total charge did not change when the time interval was as low as approximately 100 µs, and the total charge rapidly decreased when the time interval was below approximately 100 µs. Thus, it was determined that the interaction occurs within a time interval of approximately 100 µs.</description><subject>Dosage</subject><subject>Ion currents</subject><subject>Ion implantation</subject><subject>Ion sources</subject><subject>Laser beams</subject><subject>Lasers</subject><subject>Plasma</subject><subject>Repetition</subject><subject>Scientific apparatus & instruments</subject><issn>0034-6748</issn><issn>1089-7623</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2020</creationdate><recordtype>article</recordtype><recordid>eNp90MtKAzEUBuAgitbqwheQgBsVRnOZZJKlFC-FghtdD2nmTBuZm8m04NubdqqCgtmEnHycnPwInVFyQ4nkt_RGUE601ntoRInSSSYZ30cjQniayCxVR-g4hDcSl6D0EB1xxoTWMh0hO23WEHq3ML1rG9yWuF8C7l0N2DU9-LWpNsWuMqE2eAEN-EGWrccGL91iiT100LttNV4CjhY83hxDu_IWTtBBaaoAp7t9jF4f7l8mT8ns-XE6uZslNtW8T6zUhdWynAuVphok59wakxZyXnBlFc3YPF4xpkxaCsMYLUShJAhFhSiMpHyMLoe-nW_fV_FXee2ChaoyDbSrkDOuMik0FzzSi1_0LY7axOmiygjlUsaZxuhqUNa3IXgo88672viPnJJ8k3xO813y0Z7vOq7mNRTf8ivqCK4HEKzrtxl-m3XrfzrlXVH-h_8-_QnUT5lj</recordid><startdate>20200301</startdate><enddate>20200301</enddate><creator>Kashiwagi, H.</creator><creator>Yamada, K.</creator><general>American Institute of Physics</general><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope><scope>7X8</scope><orcidid>https://orcid.org/0000-0003-1101-817X</orcidid><orcidid>https://orcid.org/000000031101817X</orcidid></search><sort><creationdate>20200301</creationdate><title>Investigation of the time interval of plasma generation for a high repetition rate laser ion source</title><author>Kashiwagi, H. ; Yamada, K.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c493t-c69dc96fb58449e6333caa4d6bd38c8172bb58228a4f5a221d5d86e58155da613</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2020</creationdate><topic>Dosage</topic><topic>Ion currents</topic><topic>Ion implantation</topic><topic>Ion sources</topic><topic>Laser beams</topic><topic>Lasers</topic><topic>Plasma</topic><topic>Repetition</topic><topic>Scientific apparatus & instruments</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Kashiwagi, H.</creatorcontrib><creatorcontrib>Yamada, K.</creatorcontrib><collection>PubMed</collection><collection>CrossRef</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>MEDLINE - Academic</collection><jtitle>Review of scientific instruments</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Kashiwagi, H.</au><au>Yamada, K.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Investigation of the time interval of plasma generation for a high repetition rate laser ion source</atitle><jtitle>Review of scientific instruments</jtitle><addtitle>Rev Sci Instrum</addtitle><date>2020-03-01</date><risdate>2020</risdate><volume>91</volume><issue>3</issue><spage>033305</spage><epage>033305</epage><pages>033305-033305</pages><issn>0034-6748</issn><eissn>1089-7623</eissn><coden>RSINAK</coden><abstract>To apply a laser ion source that generates a high-intensity pulsed beam to high-dose applications, such as ion implantation, a high repetition rate operation with a short pulse interval is required. However, when the pulse interval is shortened, there is a concern that a plasma, which is different from a single pulse plasma generation, may be formed due to the interaction between the preceding and following pulses. We investigated the time interval in which plasma pulses are generated without pulse-to-pulse interaction using a laser ion source with two lasers. In the experiment, a graphite target was irradiated by two laser beams (1064-nm wavelengths) with the same pulse widths (5.4 ns) and energies (15 mJ, 30 mJ, and 45 mJ) at different time intervals ranging from 1000 μs to 0 µs, and the time integrated value corresponding to the total charge amount was calculated from the measured time-of-flight signal of the generated carbon ion current. It was observed that the total charge did not change when the time interval was as low as approximately 100 µs, and the total charge rapidly decreased when the time interval was below approximately 100 µs. Thus, it was determined that the interaction occurs within a time interval of approximately 100 µs.</abstract><cop>United States</cop><pub>American Institute of Physics</pub><pmid>32259964</pmid><doi>10.1063/1.5130999</doi><tpages>5</tpages><orcidid>https://orcid.org/0000-0003-1101-817X</orcidid><orcidid>https://orcid.org/000000031101817X</orcidid></addata></record> |
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source | American Institute of Physics:Jisc Collections:Transitional Journals Agreement 2021-23 (Reading list); AIP_美国物理联合会现刊(与NSTL共建) |
subjects | Dosage Ion currents Ion implantation Ion sources Laser beams Lasers Plasma Repetition Scientific apparatus & instruments |
title | Investigation of the time interval of plasma generation for a high repetition rate laser ion source |
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