Characterization of Titanium Laser Ablation
The atomic and ionic emission lines of titanium are often studied in laser-induced breakdown spectroscopy (LIBS) investigations, partly due to the abundance and luminosity of the lines and titanium's prominence in industry. In the current study, a 13 ns pulsed Nd:YAG laser with 160 mJ per pulse...
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Veröffentlicht in: | Journal of physics. Conference series 2014-01, Vol.548 (1), p.12053-3 |
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description | The atomic and ionic emission lines of titanium are often studied in laser-induced breakdown spectroscopy (LIBS) investigations, partly due to the abundance and luminosity of the lines and titanium's prominence in industry. In the current study, a 13 ns pulsed Nd:YAG laser with 160 mJ per pulse ablates a titanium sample in laboratory air at 10 Hz. Ti III emission lines between 232 nm and 244 nm are observed at 200 ns after laser-surface interaction, utilizing a 6 ns window. Two-dimensional images are obtained, providing spectra emanating along the height of the ablation plume. A Boltzmann plot method is implemented in order to infer electron temperature as a function of height along the plume. The hottest region of the plasma tends to be further away from the sample surface and is on the order of 16000 K. |
doi_str_mv | 10.1088/1742-6596/548/1/012053 |
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In the current study, a 13 ns pulsed Nd:YAG laser with 160 mJ per pulse ablates a titanium sample in laboratory air at 10 Hz. Ti III emission lines between 232 nm and 244 nm are observed at 200 ns after laser-surface interaction, utilizing a 6 ns window. Two-dimensional images are obtained, providing spectra emanating along the height of the ablation plume. A Boltzmann plot method is implemented in order to infer electron temperature as a function of height along the plume. 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The hottest region of the plasma tends to be further away from the sample surface and is on the order of 16000 K.</description><subject>Ablation</subject><subject>Atomic beam spectroscopy</subject><subject>Electron energy</subject><subject>Electron temperature</subject><subject>Emission analysis</subject><subject>Emission spectroscopy</subject><subject>Laser ablation</subject><subject>Laser induced breakdown spectroscopy</subject><subject>Lasers</subject><subject>Luminosity</subject><subject>Neodymium lasers</subject><subject>Physics</subject><subject>Plumes</subject><subject>Semiconductor lasers</subject><subject>Spectrum analysis</subject><subject>Titanium</subject><subject>YAG lasers</subject><issn>1742-6588</issn><issn>1742-6596</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2014</creationdate><recordtype>article</recordtype><sourceid>BENPR</sourceid><recordid>eNpdkE1Lw0AQhhdRsFb_ggS8CBK7s1_ZPZZiVQh4qedlstlgSprU3eSgv96tlR6cy8zwPgzDQ8gt0EegWi-gECxX0qiFFGlbUGBU8jMyOwXnp1nrS3IV45ZSnqqYkYfVBwZ0ow_tN47t0GdDk23aEft22mUlRh-yZdX9RtfkosEu-pu_Pifv66fN6iUv355fV8syd1yJMRe68hSxkRxZ7YykQspa1BQqxrkz6Cgox7SHStacs7oRhoGTCWIOa1bwObk_3t2H4XPycbS7Njrfddj7YYoWCtAGDFUmoXf_0O0whT59Z5ksVMGNUSpR6ki5MMQYfGP3od1h-LJA7cGhPeixB1U2ObRgjw75DzfRYp4</recordid><startdate>20140101</startdate><enddate>20140101</enddate><creator>Woods, A C</creator><creator>Parigger, C G</creator><general>IOP Publishing</general><scope>AAYXX</scope><scope>CITATION</scope><scope>8FD</scope><scope>8FE</scope><scope>8FG</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>ARAPS</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>H8D</scope><scope>HCIFZ</scope><scope>L7M</scope><scope>P5Z</scope><scope>P62</scope><scope>PIMPY</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope><scope>7SP</scope><scope>7U5</scope><scope>8BQ</scope><scope>JG9</scope></search><sort><creationdate>20140101</creationdate><title>Characterization of Titanium Laser Ablation</title><author>Woods, A C ; Parigger, C G</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c364t-48be0aaf53a2dc950455d4d01b233c9ac016c28e1b5d332df4921c555d2cad273</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2014</creationdate><topic>Ablation</topic><topic>Atomic beam spectroscopy</topic><topic>Electron energy</topic><topic>Electron temperature</topic><topic>Emission analysis</topic><topic>Emission spectroscopy</topic><topic>Laser ablation</topic><topic>Laser induced breakdown spectroscopy</topic><topic>Lasers</topic><topic>Luminosity</topic><topic>Neodymium lasers</topic><topic>Physics</topic><topic>Plumes</topic><topic>Semiconductor lasers</topic><topic>Spectrum analysis</topic><topic>Titanium</topic><topic>YAG lasers</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Woods, A C</creatorcontrib><creatorcontrib>Parigger, C G</creatorcontrib><collection>CrossRef</collection><collection>Technology Research Database</collection><collection>ProQuest SciTech Collection</collection><collection>ProQuest Technology Collection</collection><collection>ProQuest Central (Alumni Edition)</collection><collection>ProQuest Central UK/Ireland</collection><collection>Advanced Technologies & Aerospace Collection</collection><collection>ProQuest Central Essentials</collection><collection>ProQuest Central</collection><collection>Technology Collection (ProQuest)</collection><collection>ProQuest One Community College</collection><collection>ProQuest Central Korea</collection><collection>Aerospace Database</collection><collection>SciTech Premium Collection</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>Advanced Technologies & Aerospace Database</collection><collection>ProQuest Advanced Technologies & Aerospace Collection</collection><collection>Publicly Available Content Database</collection><collection>ProQuest One Academic Eastern Edition (DO NOT USE)</collection><collection>ProQuest One Academic</collection><collection>ProQuest One Academic UKI Edition</collection><collection>ProQuest Central China</collection><collection>Electronics & Communications Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>METADEX</collection><collection>Materials Research Database</collection><jtitle>Journal of physics. 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Ti III emission lines between 232 nm and 244 nm are observed at 200 ns after laser-surface interaction, utilizing a 6 ns window. Two-dimensional images are obtained, providing spectra emanating along the height of the ablation plume. A Boltzmann plot method is implemented in order to infer electron temperature as a function of height along the plume. The hottest region of the plasma tends to be further away from the sample surface and is on the order of 16000 K.</abstract><cop>Bristol</cop><pub>IOP Publishing</pub><doi>10.1088/1742-6596/548/1/012053</doi><tpages>3</tpages><oa>free_for_read</oa></addata></record> |
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subjects | Ablation Atomic beam spectroscopy Electron energy Electron temperature Emission analysis Emission spectroscopy Laser ablation Laser induced breakdown spectroscopy Lasers Luminosity Neodymium lasers Physics Plumes Semiconductor lasers Spectrum analysis Titanium YAG lasers |
title | Characterization of Titanium Laser Ablation |
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