Site-specific fragmentation in condensed (CH3S)2 by sulfur K -edge photoexcitation
The site-specific fragmentation by core-to-valence resonant photoexcitation has been investigated for condensed (CH3S)2 (dimethyl disulfide). The data presented are the desorption yields of the fragment ions from multilayered (CH3S)2 around the sulfur K-edge photoexcitation as well as the x-ray abso...
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Veröffentlicht in: | The Journal of chemical physics 1996-11, Vol.105 (19), p.8858-8864 |
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description | The site-specific fragmentation by core-to-valence resonant photoexcitation has been investigated for condensed (CH3S)2 (dimethyl disulfide). The data presented are the desorption yields of the fragment ions from multilayered (CH3S)2 around the sulfur K-edge photoexcitation as well as the x-ray absorption and Auger decay spectra. The x-ray absorption spectrum exhibits the double structure of the S 1s→σ* resonance peak corresponding to the S 1s→σ*(S–S) and S 1s→σ*(S–C) photoexcitations. It was found that the S 1s→σ*(S–C) excitation is predominantly followed by the CH+3 desorption, but the CH+3 and S+ ions are desorbed in comparable intensity at the S 1s→σ*(S–S) excitation. The Auger decay spectra around the S 1s→σ* excitation revealed that there exist two kinds of sulfur KL2,3L2,3 spectator Auger decay originating from the S 1s→σ*(S–S) and S 1s→σ*(S–C) resonant excitations. The observed site-specific fragmentation is interpreted in terms of the localization of the spectator electron in each antibonding orbital, i.e., σ*(S–S) and σ*(S–C). |
doi_str_mv | 10.1063/1.472615 |
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A.</creator><creatorcontrib>Baba, Y. ; Yoshii, K. ; Sasaki, T. A.</creatorcontrib><description>The site-specific fragmentation by core-to-valence resonant photoexcitation has been investigated for condensed (CH3S)2 (dimethyl disulfide). The data presented are the desorption yields of the fragment ions from multilayered (CH3S)2 around the sulfur K-edge photoexcitation as well as the x-ray absorption and Auger decay spectra. The x-ray absorption spectrum exhibits the double structure of the S 1s→σ* resonance peak corresponding to the S 1s→σ*(S–S) and S 1s→σ*(S–C) photoexcitations. It was found that the S 1s→σ*(S–C) excitation is predominantly followed by the CH+3 desorption, but the CH+3 and S+ ions are desorbed in comparable intensity at the S 1s→σ*(S–S) excitation. The Auger decay spectra around the S 1s→σ* excitation revealed that there exist two kinds of sulfur KL2,3L2,3 spectator Auger decay originating from the S 1s→σ*(S–S) and S 1s→σ*(S–C) resonant excitations. The observed site-specific fragmentation is interpreted in terms of the localization of the spectator electron in each antibonding orbital, i.e., σ*(S–S) and σ*(S–C).</description><identifier>ISSN: 0021-9606</identifier><identifier>EISSN: 1089-7690</identifier><identifier>DOI: 10.1063/1.472615</identifier><language>eng</language><ispartof>The Journal of chemical physics, 1996-11, Vol.105 (19), p.8858-8864</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c206t-7feb22c74a97aac012e19d5e7e49b17d92f5e75147a9fc8b37589cbc571c39cf3</citedby><cites>FETCH-LOGICAL-c206t-7feb22c74a97aac012e19d5e7e49b17d92f5e75147a9fc8b37589cbc571c39cf3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27924,27925</link.rule.ids></links><search><creatorcontrib>Baba, Y.</creatorcontrib><creatorcontrib>Yoshii, K.</creatorcontrib><creatorcontrib>Sasaki, T. A.</creatorcontrib><title>Site-specific fragmentation in condensed (CH3S)2 by sulfur K -edge photoexcitation</title><title>The Journal of chemical physics</title><description>The site-specific fragmentation by core-to-valence resonant photoexcitation has been investigated for condensed (CH3S)2 (dimethyl disulfide). The data presented are the desorption yields of the fragment ions from multilayered (CH3S)2 around the sulfur K-edge photoexcitation as well as the x-ray absorption and Auger decay spectra. The x-ray absorption spectrum exhibits the double structure of the S 1s→σ* resonance peak corresponding to the S 1s→σ*(S–S) and S 1s→σ*(S–C) photoexcitations. It was found that the S 1s→σ*(S–C) excitation is predominantly followed by the CH+3 desorption, but the CH+3 and S+ ions are desorbed in comparable intensity at the S 1s→σ*(S–S) excitation. The Auger decay spectra around the S 1s→σ* excitation revealed that there exist two kinds of sulfur KL2,3L2,3 spectator Auger decay originating from the S 1s→σ*(S–S) and S 1s→σ*(S–C) resonant excitations. The observed site-specific fragmentation is interpreted in terms of the localization of the spectator electron in each antibonding orbital, i.e., σ*(S–S) and σ*(S–C).</description><issn>0021-9606</issn><issn>1089-7690</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1996</creationdate><recordtype>article</recordtype><recordid>eNotkM1Kw0AURgdRMFbBR5hlXUy9d_IzmaUEbcWCYHUdJjd36kibhEwK9u1V6urwLc63OELcIiwQivQeF5nRBeZnIkEorTKFhXORAGhUtoDiUlzF-AUAaHSWiLdNmFjFgSn4QNKPbrvnbnJT6DsZOkl913IXuZXzapVu7rRsjjIedv4wyhepuN2yHD77qedvCiftWlx4t4t888-Z-Hh6fK9Wav26fK4e1oo0FJMynhutyWTOGucIUDPaNmfDmW3QtFb735FjZpz1VDapyUtLDeUGKbXk05mYn35p7GMc2dfDGPZuPNYI9V-LGutTi_QHYAhQnQ</recordid><startdate>19961115</startdate><enddate>19961115</enddate><creator>Baba, Y.</creator><creator>Yoshii, K.</creator><creator>Sasaki, T. A.</creator><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>19961115</creationdate><title>Site-specific fragmentation in condensed (CH3S)2 by sulfur K -edge photoexcitation</title><author>Baba, Y. ; Yoshii, K. ; Sasaki, T. A.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c206t-7feb22c74a97aac012e19d5e7e49b17d92f5e75147a9fc8b37589cbc571c39cf3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1996</creationdate><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Baba, Y.</creatorcontrib><creatorcontrib>Yoshii, K.</creatorcontrib><creatorcontrib>Sasaki, T. A.</creatorcontrib><collection>CrossRef</collection><jtitle>The Journal of chemical physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Baba, Y.</au><au>Yoshii, K.</au><au>Sasaki, T. A.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Site-specific fragmentation in condensed (CH3S)2 by sulfur K -edge photoexcitation</atitle><jtitle>The Journal of chemical physics</jtitle><date>1996-11-15</date><risdate>1996</risdate><volume>105</volume><issue>19</issue><spage>8858</spage><epage>8864</epage><pages>8858-8864</pages><issn>0021-9606</issn><eissn>1089-7690</eissn><abstract>The site-specific fragmentation by core-to-valence resonant photoexcitation has been investigated for condensed (CH3S)2 (dimethyl disulfide). The data presented are the desorption yields of the fragment ions from multilayered (CH3S)2 around the sulfur K-edge photoexcitation as well as the x-ray absorption and Auger decay spectra. The x-ray absorption spectrum exhibits the double structure of the S 1s→σ* resonance peak corresponding to the S 1s→σ*(S–S) and S 1s→σ*(S–C) photoexcitations. It was found that the S 1s→σ*(S–C) excitation is predominantly followed by the CH+3 desorption, but the CH+3 and S+ ions are desorbed in comparable intensity at the S 1s→σ*(S–S) excitation. The Auger decay spectra around the S 1s→σ* excitation revealed that there exist two kinds of sulfur KL2,3L2,3 spectator Auger decay originating from the S 1s→σ*(S–S) and S 1s→σ*(S–C) resonant excitations. The observed site-specific fragmentation is interpreted in terms of the localization of the spectator electron in each antibonding orbital, i.e., σ*(S–S) and σ*(S–C).</abstract><doi>10.1063/1.472615</doi><tpages>7</tpages></addata></record> |
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title | Site-specific fragmentation in condensed (CH3S)2 by sulfur K -edge photoexcitation |
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