Raman spectroscopic properties and Raman identification of CaS‐MgS‐MnS‐FeS‐Cr 2 FeS 4 sulfides in meteorites and reduced sulfur‐rich systems
Raman spectra were acquired on a series of natural and synthetic sulfide minerals, commonly found in enstatite meteorites: oldhamite (CaS), niningerite or keilite ((Mg,Fe)S), alabandite (MnS), troilite (FeS), and daubreelite (Cr 2 FeS 4 ). Natural samples come from three enstatite chondrites, three...
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creator | Avril, Caroline Malavergne, Valérie Caracas, Razvan Zanda, Brigitte Reynard, Bruno Charon, Emeline Bobocioiu, Ema Brunet, Fabrice Borensztajn, Stephan Pont, Sylvain Tarrida, Martine Guyot, François |
description | Raman spectra were acquired on a series of natural and synthetic sulfide minerals, commonly found in enstatite meteorites: oldhamite (CaS), niningerite or keilite ((Mg,Fe)S), alabandite (MnS), troilite (FeS), and daubreelite (Cr
2
FeS
4
). Natural samples come from three enstatite chondrites, three aubrites, and one anomalous ungrouped enstatite meteorite. Synthetic samples range from pure endmembers (CaS, FeS, MgS) to complex solid solutions (Fe, Mg, Ca)S. The main Raman peaks are localized at 225, 285, 360, and 470 cm
−1
for the Mg‐rich sulfides; at 185, 205, and 285 cm
−1
for the Ca‐rich sulfides; at 250, 370, and 580 cm
−1
for the Mn‐rich sulfides; at 255, 290, and 365 cm
−1
for the Cr‐rich sulfides; and at 290 and 335 cm
−1
for troilite with, occasionally, an extra peak at 240 cm
−1
. A peak at 160 cm
−1
is present in all Raman spectra and cannot be used to discriminate between the different sulfide compositions. According to group theory, none of the cubic monosulfides oldhamite, niningerite, or alabandite should present first‐order Raman spectra because of their ideal rocksalt structure. The occurrence of broad Raman peaks is tentatively explained by local breaking of symmetry rules. Measurements compare well with the infrared frequencies calculated from first‐principles calculations. Raman spectra arise from activation of certain vibrational modes due to clustering in the solid solutions or to coupling with electronic transitions in semiconductor sulfides. |
doi_str_mv | 10.1111/maps.12145 |
format | Article |
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2
FeS
4
). Natural samples come from three enstatite chondrites, three aubrites, and one anomalous ungrouped enstatite meteorite. Synthetic samples range from pure endmembers (CaS, FeS, MgS) to complex solid solutions (Fe, Mg, Ca)S. The main Raman peaks are localized at 225, 285, 360, and 470 cm
−1
for the Mg‐rich sulfides; at 185, 205, and 285 cm
−1
for the Ca‐rich sulfides; at 250, 370, and 580 cm
−1
for the Mn‐rich sulfides; at 255, 290, and 365 cm
−1
for the Cr‐rich sulfides; and at 290 and 335 cm
−1
for troilite with, occasionally, an extra peak at 240 cm
−1
. A peak at 160 cm
−1
is present in all Raman spectra and cannot be used to discriminate between the different sulfide compositions. According to group theory, none of the cubic monosulfides oldhamite, niningerite, or alabandite should present first‐order Raman spectra because of their ideal rocksalt structure. The occurrence of broad Raman peaks is tentatively explained by local breaking of symmetry rules. Measurements compare well with the infrared frequencies calculated from first‐principles calculations. Raman spectra arise from activation of certain vibrational modes due to clustering in the solid solutions or to coupling with electronic transitions in semiconductor sulfides.</description><identifier>ISSN: 1086-9379</identifier><identifier>EISSN: 1945-5100</identifier><identifier>DOI: 10.1111/maps.12145</identifier><language>eng</language><publisher>Wiley</publisher><subject>Earth Sciences ; Mineralogy ; Sciences of the Universe</subject><ispartof>Meteoritics & planetary science, 2013-08, Vol.48 (8), p.1415-1426</ispartof><rights>Distributed under a Creative Commons Attribution 4.0 International License</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c1101-c29792775ff888702fb989147c59eb679c0f7939fe62dd8f9c1126ff2ecbcc813</citedby><cites>FETCH-LOGICAL-c1101-c29792775ff888702fb989147c59eb679c0f7939fe62dd8f9c1126ff2ecbcc813</cites><orcidid>0000-0002-4210-7151 ; 0000-0001-5919-8363 ; 0000-0003-4622-2218 ; 0000-0003-2034-9528 ; 0000-0003-4586-776X ; 0000-0002-0929-8398 ; 0000-0002-4782-6163</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://hal.science/hal-02107398$$DView record in HAL$$Hfree_for_read</backlink></links><search><creatorcontrib>Avril, Caroline</creatorcontrib><creatorcontrib>Malavergne, Valérie</creatorcontrib><creatorcontrib>Caracas, Razvan</creatorcontrib><creatorcontrib>Zanda, Brigitte</creatorcontrib><creatorcontrib>Reynard, Bruno</creatorcontrib><creatorcontrib>Charon, Emeline</creatorcontrib><creatorcontrib>Bobocioiu, Ema</creatorcontrib><creatorcontrib>Brunet, Fabrice</creatorcontrib><creatorcontrib>Borensztajn, Stephan</creatorcontrib><creatorcontrib>Pont, Sylvain</creatorcontrib><creatorcontrib>Tarrida, Martine</creatorcontrib><creatorcontrib>Guyot, François</creatorcontrib><title>Raman spectroscopic properties and Raman identification of CaS‐MgS‐MnS‐FeS‐Cr 2 FeS 4 sulfides in meteorites and reduced sulfur‐rich systems</title><title>Meteoritics & planetary science</title><description>Raman spectra were acquired on a series of natural and synthetic sulfide minerals, commonly found in enstatite meteorites: oldhamite (CaS), niningerite or keilite ((Mg,Fe)S), alabandite (MnS), troilite (FeS), and daubreelite (Cr
2
FeS
4
). Natural samples come from three enstatite chondrites, three aubrites, and one anomalous ungrouped enstatite meteorite. Synthetic samples range from pure endmembers (CaS, FeS, MgS) to complex solid solutions (Fe, Mg, Ca)S. The main Raman peaks are localized at 225, 285, 360, and 470 cm
−1
for the Mg‐rich sulfides; at 185, 205, and 285 cm
−1
for the Ca‐rich sulfides; at 250, 370, and 580 cm
−1
for the Mn‐rich sulfides; at 255, 290, and 365 cm
−1
for the Cr‐rich sulfides; and at 290 and 335 cm
−1
for troilite with, occasionally, an extra peak at 240 cm
−1
. A peak at 160 cm
−1
is present in all Raman spectra and cannot be used to discriminate between the different sulfide compositions. According to group theory, none of the cubic monosulfides oldhamite, niningerite, or alabandite should present first‐order Raman spectra because of their ideal rocksalt structure. The occurrence of broad Raman peaks is tentatively explained by local breaking of symmetry rules. Measurements compare well with the infrared frequencies calculated from first‐principles calculations. Raman spectra arise from activation of certain vibrational modes due to clustering in the solid solutions or to coupling with electronic transitions in semiconductor sulfides.</description><subject>Earth Sciences</subject><subject>Mineralogy</subject><subject>Sciences of the Universe</subject><issn>1086-9379</issn><issn>1945-5100</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2013</creationdate><recordtype>article</recordtype><recordid>eNo9kM1KAzEUhYMoWKsbnyBbhalJ5ifJsgy2FSqCP-uQZm5spDMZkqnQnY_gygf0SZxpi3dx7uXynbM4CF1TMqH93NW6jRPKaJafoBGVWZ7klJDT_iaiSGTK5Tm6iPGDkDSnaTZCP8-61g2OLZgu-Gh86wxug28hdA4i1k2FD4iroOmcdUZ3zjfYW1zql9-v78f3vTaDzmDQMmCG-xNnOG43tjdG7BpcQwc-uO6YGqDaGqj2yDb0tuDMGsdd7KCOl-jM6k2Eq-Meo7fZ_Wu5SJZP84dyukwMpYQmhkkuGee5tUIITphdSSFpxk0uYVVwaYjlMpUWClZVwsrexgprGZiVMYKmY3RzyF3rjWqDq3XYKa-dWkyXavgRRglPpfgc2NsDa_qiYgD7b6BEDe2roX21bz_9A78efg8</recordid><startdate>201308</startdate><enddate>201308</enddate><creator>Avril, Caroline</creator><creator>Malavergne, Valérie</creator><creator>Caracas, Razvan</creator><creator>Zanda, Brigitte</creator><creator>Reynard, Bruno</creator><creator>Charon, Emeline</creator><creator>Bobocioiu, Ema</creator><creator>Brunet, Fabrice</creator><creator>Borensztajn, Stephan</creator><creator>Pont, Sylvain</creator><creator>Tarrida, Martine</creator><creator>Guyot, François</creator><general>Wiley</general><scope>AAYXX</scope><scope>CITATION</scope><scope>1XC</scope><orcidid>https://orcid.org/0000-0002-4210-7151</orcidid><orcidid>https://orcid.org/0000-0001-5919-8363</orcidid><orcidid>https://orcid.org/0000-0003-4622-2218</orcidid><orcidid>https://orcid.org/0000-0003-2034-9528</orcidid><orcidid>https://orcid.org/0000-0003-4586-776X</orcidid><orcidid>https://orcid.org/0000-0002-0929-8398</orcidid><orcidid>https://orcid.org/0000-0002-4782-6163</orcidid></search><sort><creationdate>201308</creationdate><title>Raman spectroscopic properties and Raman identification of CaS‐MgS‐MnS‐FeS‐Cr 2 FeS 4 sulfides in meteorites and reduced sulfur‐rich systems</title><author>Avril, Caroline ; Malavergne, Valérie ; Caracas, Razvan ; Zanda, Brigitte ; Reynard, Bruno ; Charon, Emeline ; Bobocioiu, Ema ; Brunet, Fabrice ; Borensztajn, Stephan ; Pont, Sylvain ; Tarrida, Martine ; Guyot, François</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c1101-c29792775ff888702fb989147c59eb679c0f7939fe62dd8f9c1126ff2ecbcc813</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2013</creationdate><topic>Earth Sciences</topic><topic>Mineralogy</topic><topic>Sciences of the Universe</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Avril, Caroline</creatorcontrib><creatorcontrib>Malavergne, Valérie</creatorcontrib><creatorcontrib>Caracas, Razvan</creatorcontrib><creatorcontrib>Zanda, Brigitte</creatorcontrib><creatorcontrib>Reynard, Bruno</creatorcontrib><creatorcontrib>Charon, Emeline</creatorcontrib><creatorcontrib>Bobocioiu, Ema</creatorcontrib><creatorcontrib>Brunet, Fabrice</creatorcontrib><creatorcontrib>Borensztajn, Stephan</creatorcontrib><creatorcontrib>Pont, Sylvain</creatorcontrib><creatorcontrib>Tarrida, Martine</creatorcontrib><creatorcontrib>Guyot, François</creatorcontrib><collection>CrossRef</collection><collection>Hyper Article en Ligne (HAL)</collection><jtitle>Meteoritics & planetary science</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Avril, Caroline</au><au>Malavergne, Valérie</au><au>Caracas, Razvan</au><au>Zanda, Brigitte</au><au>Reynard, Bruno</au><au>Charon, Emeline</au><au>Bobocioiu, Ema</au><au>Brunet, Fabrice</au><au>Borensztajn, Stephan</au><au>Pont, Sylvain</au><au>Tarrida, Martine</au><au>Guyot, François</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Raman spectroscopic properties and Raman identification of CaS‐MgS‐MnS‐FeS‐Cr 2 FeS 4 sulfides in meteorites and reduced sulfur‐rich systems</atitle><jtitle>Meteoritics & planetary science</jtitle><date>2013-08</date><risdate>2013</risdate><volume>48</volume><issue>8</issue><spage>1415</spage><epage>1426</epage><pages>1415-1426</pages><issn>1086-9379</issn><eissn>1945-5100</eissn><abstract>Raman spectra were acquired on a series of natural and synthetic sulfide minerals, commonly found in enstatite meteorites: oldhamite (CaS), niningerite or keilite ((Mg,Fe)S), alabandite (MnS), troilite (FeS), and daubreelite (Cr
2
FeS
4
). Natural samples come from three enstatite chondrites, three aubrites, and one anomalous ungrouped enstatite meteorite. Synthetic samples range from pure endmembers (CaS, FeS, MgS) to complex solid solutions (Fe, Mg, Ca)S. The main Raman peaks are localized at 225, 285, 360, and 470 cm
−1
for the Mg‐rich sulfides; at 185, 205, and 285 cm
−1
for the Ca‐rich sulfides; at 250, 370, and 580 cm
−1
for the Mn‐rich sulfides; at 255, 290, and 365 cm
−1
for the Cr‐rich sulfides; and at 290 and 335 cm
−1
for troilite with, occasionally, an extra peak at 240 cm
−1
. A peak at 160 cm
−1
is present in all Raman spectra and cannot be used to discriminate between the different sulfide compositions. According to group theory, none of the cubic monosulfides oldhamite, niningerite, or alabandite should present first‐order Raman spectra because of their ideal rocksalt structure. The occurrence of broad Raman peaks is tentatively explained by local breaking of symmetry rules. Measurements compare well with the infrared frequencies calculated from first‐principles calculations. Raman spectra arise from activation of certain vibrational modes due to clustering in the solid solutions or to coupling with electronic transitions in semiconductor sulfides.</abstract><pub>Wiley</pub><doi>10.1111/maps.12145</doi><tpages>12</tpages><orcidid>https://orcid.org/0000-0002-4210-7151</orcidid><orcidid>https://orcid.org/0000-0001-5919-8363</orcidid><orcidid>https://orcid.org/0000-0003-4622-2218</orcidid><orcidid>https://orcid.org/0000-0003-2034-9528</orcidid><orcidid>https://orcid.org/0000-0003-4586-776X</orcidid><orcidid>https://orcid.org/0000-0002-0929-8398</orcidid><orcidid>https://orcid.org/0000-0002-4782-6163</orcidid></addata></record> |
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source | Wiley Free Content; Wiley Online Library Journals Frontfile Complete; Elektronische Zeitschriftenbibliothek - Frei zugängliche E-Journals |
subjects | Earth Sciences Mineralogy Sciences of the Universe |
title | Raman spectroscopic properties and Raman identification of CaS‐MgS‐MnS‐FeS‐Cr 2 FeS 4 sulfides in meteorites and reduced sulfur‐rich systems |
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