Photoionized plasmas induced in neon with extreme ultraviolet and soft X-ray pulses produced using low and high energy laser systems
A comparative study of photoionized plasmas created by two soft X-ray and extreme ultraviolet (SXR/EUV) laser plasma sources with different parameters is presented. The two sources are based on double-stream Xe/He gas-puff targets irradiated with high (500 J/0.3 ns) and low energy (10 J/1 ns) laser...
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| Veröffentlicht in: | Physics of plasmas 2015-04, Vol.22 (4) |
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| creator | Bartnik, A. Wachulak, P. Fok, T. Węgrzyński, Ł. Fiedorowicz, H. Pisarczyk, T. Chodukowski, T. Kalinowska, Z. Dudzak, R. Dostal, J. Krousky, E. Skala, J. Ullschmied, J. Hrebicek, J. Medrik, T. |
| description | A comparative study of photoionized plasmas created by two soft X-ray and extreme ultraviolet (SXR/EUV) laser plasma sources with different parameters is presented. The two sources are based on double-stream Xe/He gas-puff targets irradiated with high (500 J/0.3 ns) and low energy (10 J/1 ns) laser pulses. In both cases, the SXR/EUV beam irradiated the gas stream, injected into a vacuum chamber synchronously with the radiation pulse. Irradiation of gases resulted in formation of photoionized plasmas emitting radiation in the SXR/EUV range. The measured Ne plasma radiation spectra are dominated by emission lines corresponding to radiative transitions in singly charged ions. A significant difference concerns origin of the lines: K-shell or L-shell emissions occur in case of the high and low energy irradiating system, respectively. In high energy system, the electron density measurements were also performed by laser interferometry, employing a femtosecond laser system. A maximum electron density for Ne plasma reached the value of 2·1018 cm−3. For the low energy system, a detection limit was too high for the interferometric measurements, thus only an upper estimation for electron density could be made. |
| doi_str_mv | 10.1063/1.4919024 |
| format | Article |
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The two sources are based on double-stream Xe/He gas-puff targets irradiated with high (500 J/0.3 ns) and low energy (10 J/1 ns) laser pulses. In both cases, the SXR/EUV beam irradiated the gas stream, injected into a vacuum chamber synchronously with the radiation pulse. Irradiation of gases resulted in formation of photoionized plasmas emitting radiation in the SXR/EUV range. The measured Ne plasma radiation spectra are dominated by emission lines corresponding to radiative transitions in singly charged ions. A significant difference concerns origin of the lines: K-shell or L-shell emissions occur in case of the high and low energy irradiating system, respectively. In high energy system, the electron density measurements were also performed by laser interferometry, employing a femtosecond laser system. A maximum electron density for Ne plasma reached the value of 2·1018 cm−3. For the low energy system, a detection limit was too high for the interferometric measurements, thus only an upper estimation for electron density could be made.</description><identifier>ISSN: 1070-664X</identifier><identifier>EISSN: 1089-7674</identifier><identifier>DOI: 10.1063/1.4919024</identifier><language>eng</language><publisher>Melville: American Institute of Physics</publisher><subject>70 PLASMA PHYSICS AND FUSION TECHNOLOGY ; Comparative studies ; ELECTRON DENSITY ; Electron density measurement ; Emission spectra ; EXTREME ULTRAVIOLET RADIATION ; Femtosecond pulsed lasers ; HELIUM ; INTERFEROMETRY ; IONS ; Irradiation ; K SHELL ; L SHELL ; Laser beams ; Laser interferometry ; Laser plasmas ; LASER-PRODUCED PLASMA ; Lasers ; NEON ; PHOTOIONIZATION ; PHOTON BEAMS ; Plasma ; Plasma physics ; Plasma radiation ; PULSED IRRADIATION ; Radiation spectra ; Rangefinding ; SENSITIVITY ; SOFT X RADIATION ; Soft x rays ; SPECTRA ; Vacuum chambers ; X ray spectra ; X-RAY LASERS ; XENON</subject><ispartof>Physics of plasmas, 2015-04, Vol.22 (4)</ispartof><rights>2015 AIP Publishing LLC.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c285t-1169c968f233fc8ced4d3b676e7b66882868786ba262d0acefdd0691246cdb823</citedby><cites>FETCH-LOGICAL-c285t-1169c968f233fc8ced4d3b676e7b66882868786ba262d0acefdd0691246cdb823</cites><orcidid>0000-0002-2012-7450 ; 0000-0001-9971-7201 ; 0000-0001-9853-7946</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>230,314,776,780,881,27901,27902</link.rule.ids><backlink>$$Uhttps://www.osti.gov/biblio/22408360$$D View this record in Osti.gov$$Hfree_for_read</backlink></links><search><creatorcontrib>Bartnik, A.</creatorcontrib><creatorcontrib>Wachulak, P.</creatorcontrib><creatorcontrib>Fok, T.</creatorcontrib><creatorcontrib>Węgrzyński, Ł.</creatorcontrib><creatorcontrib>Fiedorowicz, H.</creatorcontrib><creatorcontrib>Pisarczyk, T.</creatorcontrib><creatorcontrib>Chodukowski, T.</creatorcontrib><creatorcontrib>Kalinowska, Z.</creatorcontrib><creatorcontrib>Dudzak, R.</creatorcontrib><creatorcontrib>Dostal, J.</creatorcontrib><creatorcontrib>Krousky, E.</creatorcontrib><creatorcontrib>Skala, J.</creatorcontrib><creatorcontrib>Ullschmied, J.</creatorcontrib><creatorcontrib>Hrebicek, J.</creatorcontrib><creatorcontrib>Medrik, T.</creatorcontrib><title>Photoionized plasmas induced in neon with extreme ultraviolet and soft X-ray pulses produced using low and high energy laser systems</title><title>Physics of plasmas</title><description>A comparative study of photoionized plasmas created by two soft X-ray and extreme ultraviolet (SXR/EUV) laser plasma sources with different parameters is presented. The two sources are based on double-stream Xe/He gas-puff targets irradiated with high (500 J/0.3 ns) and low energy (10 J/1 ns) laser pulses. In both cases, the SXR/EUV beam irradiated the gas stream, injected into a vacuum chamber synchronously with the radiation pulse. Irradiation of gases resulted in formation of photoionized plasmas emitting radiation in the SXR/EUV range. The measured Ne plasma radiation spectra are dominated by emission lines corresponding to radiative transitions in singly charged ions. A significant difference concerns origin of the lines: K-shell or L-shell emissions occur in case of the high and low energy irradiating system, respectively. In high energy system, the electron density measurements were also performed by laser interferometry, employing a femtosecond laser system. A maximum electron density for Ne plasma reached the value of 2·1018 cm−3. For the low energy system, a detection limit was too high for the interferometric measurements, thus only an upper estimation for electron density could be made.</description><subject>70 PLASMA PHYSICS AND FUSION TECHNOLOGY</subject><subject>Comparative studies</subject><subject>ELECTRON DENSITY</subject><subject>Electron density measurement</subject><subject>Emission spectra</subject><subject>EXTREME ULTRAVIOLET RADIATION</subject><subject>Femtosecond pulsed lasers</subject><subject>HELIUM</subject><subject>INTERFEROMETRY</subject><subject>IONS</subject><subject>Irradiation</subject><subject>K SHELL</subject><subject>L SHELL</subject><subject>Laser beams</subject><subject>Laser interferometry</subject><subject>Laser plasmas</subject><subject>LASER-PRODUCED PLASMA</subject><subject>Lasers</subject><subject>NEON</subject><subject>PHOTOIONIZATION</subject><subject>PHOTON BEAMS</subject><subject>Plasma</subject><subject>Plasma physics</subject><subject>Plasma radiation</subject><subject>PULSED IRRADIATION</subject><subject>Radiation spectra</subject><subject>Rangefinding</subject><subject>SENSITIVITY</subject><subject>SOFT X RADIATION</subject><subject>Soft x rays</subject><subject>SPECTRA</subject><subject>Vacuum chambers</subject><subject>X ray spectra</subject><subject>X-RAY LASERS</subject><subject>XENON</subject><issn>1070-664X</issn><issn>1089-7674</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2015</creationdate><recordtype>article</recordtype><recordid>eNpFkT9PwzAQxSMEEqUw8A0sMTGk2E56cUZU8U-qBANI3SzHcRpXqR1sBwgzHxyXVmK6O-m937vTJcklwTOCIbshs7wkJab5UTIhmJVpAUV-vOsLnALkq9PkzPsNxjiHOZskPy-tDVZbo79VjfpO-K3wSJt6kHHWBhllDfrUoUXqKzi1VWjoghMf2nYqIGFq5G0T0Cp1YkT90HnlUe_s3j94bdaos59_wlavI8Uotx5RDFIO-dEHtfXnyUkjovPiUKfJ2_3d6-IxXT4_PC1ul6mkbB5SQqCUJbCGZlkjWQzI66yCAlRRATBGGbCCQSUo0BoLqZq6xlASmoOsK0azaXK151ofNPdSByVbaY1RMnBKc8wywP-qeMb7oHzgGzs4ExfjNLIYjvgsqq73Kums9041vHd6K9zICea7V3DCD6_IfgHMTnye</recordid><startdate>20150401</startdate><enddate>20150401</enddate><creator>Bartnik, A.</creator><creator>Wachulak, P.</creator><creator>Fok, T.</creator><creator>Węgrzyński, Ł.</creator><creator>Fiedorowicz, H.</creator><creator>Pisarczyk, T.</creator><creator>Chodukowski, T.</creator><creator>Kalinowska, Z.</creator><creator>Dudzak, R.</creator><creator>Dostal, J.</creator><creator>Krousky, E.</creator><creator>Skala, J.</creator><creator>Ullschmied, J.</creator><creator>Hrebicek, J.</creator><creator>Medrik, T.</creator><general>American Institute of Physics</general><scope>AAYXX</scope><scope>CITATION</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope><scope>OTOTI</scope><orcidid>https://orcid.org/0000-0002-2012-7450</orcidid><orcidid>https://orcid.org/0000-0001-9971-7201</orcidid><orcidid>https://orcid.org/0000-0001-9853-7946</orcidid></search><sort><creationdate>20150401</creationdate><title>Photoionized plasmas induced in neon with extreme ultraviolet and soft X-ray pulses produced using low and high energy laser systems</title><author>Bartnik, A. ; Wachulak, P. ; Fok, T. ; Węgrzyński, Ł. ; Fiedorowicz, H. ; Pisarczyk, T. ; Chodukowski, T. ; Kalinowska, Z. ; Dudzak, R. ; Dostal, J. ; Krousky, E. ; Skala, J. ; Ullschmied, J. ; Hrebicek, J. ; Medrik, T.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c285t-1169c968f233fc8ced4d3b676e7b66882868786ba262d0acefdd0691246cdb823</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2015</creationdate><topic>70 PLASMA PHYSICS AND FUSION TECHNOLOGY</topic><topic>Comparative studies</topic><topic>ELECTRON DENSITY</topic><topic>Electron density measurement</topic><topic>Emission spectra</topic><topic>EXTREME ULTRAVIOLET RADIATION</topic><topic>Femtosecond pulsed lasers</topic><topic>HELIUM</topic><topic>INTERFEROMETRY</topic><topic>IONS</topic><topic>Irradiation</topic><topic>K SHELL</topic><topic>L SHELL</topic><topic>Laser beams</topic><topic>Laser interferometry</topic><topic>Laser plasmas</topic><topic>LASER-PRODUCED PLASMA</topic><topic>Lasers</topic><topic>NEON</topic><topic>PHOTOIONIZATION</topic><topic>PHOTON BEAMS</topic><topic>Plasma</topic><topic>Plasma physics</topic><topic>Plasma radiation</topic><topic>PULSED IRRADIATION</topic><topic>Radiation spectra</topic><topic>Rangefinding</topic><topic>SENSITIVITY</topic><topic>SOFT X RADIATION</topic><topic>Soft x rays</topic><topic>SPECTRA</topic><topic>Vacuum chambers</topic><topic>X ray spectra</topic><topic>X-RAY LASERS</topic><topic>XENON</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Bartnik, A.</creatorcontrib><creatorcontrib>Wachulak, P.</creatorcontrib><creatorcontrib>Fok, T.</creatorcontrib><creatorcontrib>Węgrzyński, Ł.</creatorcontrib><creatorcontrib>Fiedorowicz, H.</creatorcontrib><creatorcontrib>Pisarczyk, T.</creatorcontrib><creatorcontrib>Chodukowski, T.</creatorcontrib><creatorcontrib>Kalinowska, Z.</creatorcontrib><creatorcontrib>Dudzak, R.</creatorcontrib><creatorcontrib>Dostal, J.</creatorcontrib><creatorcontrib>Krousky, E.</creatorcontrib><creatorcontrib>Skala, J.</creatorcontrib><creatorcontrib>Ullschmied, J.</creatorcontrib><creatorcontrib>Hrebicek, J.</creatorcontrib><creatorcontrib>Medrik, T.</creatorcontrib><collection>CrossRef</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>OSTI.GOV</collection><jtitle>Physics of plasmas</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Bartnik, A.</au><au>Wachulak, P.</au><au>Fok, T.</au><au>Węgrzyński, Ł.</au><au>Fiedorowicz, H.</au><au>Pisarczyk, T.</au><au>Chodukowski, T.</au><au>Kalinowska, Z.</au><au>Dudzak, R.</au><au>Dostal, J.</au><au>Krousky, E.</au><au>Skala, J.</au><au>Ullschmied, J.</au><au>Hrebicek, J.</au><au>Medrik, T.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Photoionized plasmas induced in neon with extreme ultraviolet and soft X-ray pulses produced using low and high energy laser systems</atitle><jtitle>Physics of plasmas</jtitle><date>2015-04-01</date><risdate>2015</risdate><volume>22</volume><issue>4</issue><issn>1070-664X</issn><eissn>1089-7674</eissn><abstract>A comparative study of photoionized plasmas created by two soft X-ray and extreme ultraviolet (SXR/EUV) laser plasma sources with different parameters is presented. The two sources are based on double-stream Xe/He gas-puff targets irradiated with high (500 J/0.3 ns) and low energy (10 J/1 ns) laser pulses. In both cases, the SXR/EUV beam irradiated the gas stream, injected into a vacuum chamber synchronously with the radiation pulse. Irradiation of gases resulted in formation of photoionized plasmas emitting radiation in the SXR/EUV range. The measured Ne plasma radiation spectra are dominated by emission lines corresponding to radiative transitions in singly charged ions. A significant difference concerns origin of the lines: K-shell or L-shell emissions occur in case of the high and low energy irradiating system, respectively. In high energy system, the electron density measurements were also performed by laser interferometry, employing a femtosecond laser system. A maximum electron density for Ne plasma reached the value of 2·1018 cm−3. For the low energy system, a detection limit was too high for the interferometric measurements, thus only an upper estimation for electron density could be made.</abstract><cop>Melville</cop><pub>American Institute of Physics</pub><doi>10.1063/1.4919024</doi><orcidid>https://orcid.org/0000-0002-2012-7450</orcidid><orcidid>https://orcid.org/0000-0001-9971-7201</orcidid><orcidid>https://orcid.org/0000-0001-9853-7946</orcidid></addata></record> |
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| subjects | 70 PLASMA PHYSICS AND FUSION TECHNOLOGY Comparative studies ELECTRON DENSITY Electron density measurement Emission spectra EXTREME ULTRAVIOLET RADIATION Femtosecond pulsed lasers HELIUM INTERFEROMETRY IONS Irradiation K SHELL L SHELL Laser beams Laser interferometry Laser plasmas LASER-PRODUCED PLASMA Lasers NEON PHOTOIONIZATION PHOTON BEAMS Plasma Plasma physics Plasma radiation PULSED IRRADIATION Radiation spectra Rangefinding SENSITIVITY SOFT X RADIATION Soft x rays SPECTRA Vacuum chambers X ray spectra X-RAY LASERS XENON |
| title | Photoionized plasmas induced in neon with extreme ultraviolet and soft X-ray pulses produced using low and high energy laser systems |
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