From Metallic LnTt (Ln = La, Nd; Tt = Si, Ge, Sn) to Electron‐precise Zintl Phase Hydrides LnTtH
LnTt (Ln = La, Nd; Tt = Si, Ge, Sn) compounds crystallize in the CrB‐ or the FeB‐structure type with 1∞[Tt2–]‐polyanionic zigzag chains and can be rationalized as Ln3+Tt2–e–. They take up hydrogen at gas pressures from 10 to 160 bar and temperatures up to 750 K. The hydrides LnTtH1–x (0.04 ≤ x ≤ 0.3...
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Veröffentlicht in: | Zeitschrift für anorganische und allgemeine Chemie (1950) 2018-11, Vol.644 (22), p.1532-1539 |
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description | LnTt (Ln = La, Nd; Tt = Si, Ge, Sn) compounds crystallize in the CrB‐ or the FeB‐structure type with 1∞[Tt2–]‐polyanionic zigzag chains and can be rationalized as Ln3+Tt2–e–. They take up hydrogen at gas pressures from 10 to 160 bar and temperatures up to 750 K. The hydrides LnTtH1–x (0.04 ≤ x ≤ 0.39) crystallize either in a hydrogen filled CrB‐structure type (ZrNiH type, C‐phase, Cmcm: LaSiD0.92(1), LaGeD0.88(1), NdSiD, NdGeD0.95(1), LaSnHx) or in a hydrogen filled FeB‐structure type (LaGeH type, P‐phase, Pnma: LaSiD0.61(3), LaGeD0.96(4), NdSiD0.88(6)). In both cases, hydrogen atoms partially fill tetrahedral Ln4 voids as proven by neutron powder diffraction. While CrB‐structure type LnTt reacts to C‐phase only, FeB‐structure type LnTt hydrogenates to mixtures of C‐ (major phase) and P‐type hydrides. Electronic structure calculations reveal the depopulation of Ln‐d states, which cause the metallic conductivity in LnTt to be the main electronic effect upon hydrogenation. They further suggest Zintl phase hydrides LnTtH to be still poor metallic conductors with a pseudo bandgap at the Fermi level. The hydrogenation reaction from LnTt to LnTtH may thus be regarded as an incomplete metal to semiconductor transition. |
doi_str_mv | 10.1002/zaac.201800062 |
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They take up hydrogen at gas pressures from 10 to 160 bar and temperatures up to 750 K. The hydrides LnTtH1–x (0.04 ≤ x ≤ 0.39) crystallize either in a hydrogen filled CrB‐structure type (ZrNiH type, C‐phase, Cmcm: LaSiD0.92(1), LaGeD0.88(1), NdSiD, NdGeD0.95(1), LaSnHx) or in a hydrogen filled FeB‐structure type (LaGeH type, P‐phase, Pnma: LaSiD0.61(3), LaGeD0.96(4), NdSiD0.88(6)). In both cases, hydrogen atoms partially fill tetrahedral Ln4 voids as proven by neutron powder diffraction. While CrB‐structure type LnTt reacts to C‐phase only, FeB‐structure type LnTt hydrogenates to mixtures of C‐ (major phase) and P‐type hydrides. Electronic structure calculations reveal the depopulation of Ln‐d states, which cause the metallic conductivity in LnTt to be the main electronic effect upon hydrogenation. They further suggest Zintl phase hydrides LnTtH to be still poor metallic conductors with a pseudo bandgap at the Fermi level. The hydrogenation reaction from LnTt to LnTtH may thus be regarded as an incomplete metal to semiconductor transition.</description><identifier>ISSN: 0044-2313</identifier><identifier>EISSN: 1521-3749</identifier><identifier>DOI: 10.1002/zaac.201800062</identifier><language>eng</language><publisher>Weinheim: Wiley Subscription Services, Inc</publisher><subject>Conductors ; DFT calculation ; Electronic structure ; Germanium ; Hydrides ; Hydrogen ; Hydrogen atoms ; Hydrogen storage ; Hydrogenation ; Lanthanides ; Metal hydrides ; Neodymium ; Neutron diffraction ; Quantum theory ; Silicon compounds ; Tin ; Zintl phases</subject><ispartof>Zeitschrift für anorganische und allgemeine Chemie (1950), 2018-11, Vol.644 (22), p.1532-1539</ispartof><rights>2018 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://onlinelibrary.wiley.com/doi/pdf/10.1002%2Fzaac.201800062$$EPDF$$P50$$Gwiley$$H</linktopdf><linktohtml>$$Uhttps://onlinelibrary.wiley.com/doi/full/10.1002%2Fzaac.201800062$$EHTML$$P50$$Gwiley$$H</linktohtml><link.rule.ids>314,776,780,1411,27903,27904,45553,45554</link.rule.ids></links><search><creatorcontrib>Werwein, Anton</creatorcontrib><creatorcontrib>Auer, Henry</creatorcontrib><creatorcontrib>Kuske, Lena</creatorcontrib><creatorcontrib>Kohlmann, Holger</creatorcontrib><title>From Metallic LnTt (Ln = La, Nd; Tt = Si, Ge, Sn) to Electron‐precise Zintl Phase Hydrides LnTtH</title><title>Zeitschrift für anorganische und allgemeine Chemie (1950)</title><description>LnTt (Ln = La, Nd; Tt = Si, Ge, Sn) compounds crystallize in the CrB‐ or the FeB‐structure type with 1∞[Tt2–]‐polyanionic zigzag chains and can be rationalized as Ln3+Tt2–e–. They take up hydrogen at gas pressures from 10 to 160 bar and temperatures up to 750 K. The hydrides LnTtH1–x (0.04 ≤ x ≤ 0.39) crystallize either in a hydrogen filled CrB‐structure type (ZrNiH type, C‐phase, Cmcm: LaSiD0.92(1), LaGeD0.88(1), NdSiD, NdGeD0.95(1), LaSnHx) or in a hydrogen filled FeB‐structure type (LaGeH type, P‐phase, Pnma: LaSiD0.61(3), LaGeD0.96(4), NdSiD0.88(6)). In both cases, hydrogen atoms partially fill tetrahedral Ln4 voids as proven by neutron powder diffraction. While CrB‐structure type LnTt reacts to C‐phase only, FeB‐structure type LnTt hydrogenates to mixtures of C‐ (major phase) and P‐type hydrides. Electronic structure calculations reveal the depopulation of Ln‐d states, which cause the metallic conductivity in LnTt to be the main electronic effect upon hydrogenation. They further suggest Zintl phase hydrides LnTtH to be still poor metallic conductors with a pseudo bandgap at the Fermi level. The hydrogenation reaction from LnTt to LnTtH may thus be regarded as an incomplete metal to semiconductor transition.</description><subject>Conductors</subject><subject>DFT calculation</subject><subject>Electronic structure</subject><subject>Germanium</subject><subject>Hydrides</subject><subject>Hydrogen</subject><subject>Hydrogen atoms</subject><subject>Hydrogen storage</subject><subject>Hydrogenation</subject><subject>Lanthanides</subject><subject>Metal hydrides</subject><subject>Neodymium</subject><subject>Neutron diffraction</subject><subject>Quantum theory</subject><subject>Silicon compounds</subject><subject>Tin</subject><subject>Zintl phases</subject><issn>0044-2313</issn><issn>1521-3749</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2018</creationdate><recordtype>article</recordtype><sourceid/><recordid>eNo9kMtKw0AUhgdRsFa3rgfcKDT1zK3TQboopRchXqB1080wmUwwJU3iJKXUlY_gM_okpla6OreP_8CH0DWBLgGg95_G2C4F0geAHj1BLSIoCZjk6hS1ADgPKCPsHF1U1apBCAjRQtHEF2v85GqTZanFYb6o8W2Y4wEOTQc_xw-4WQzwPO3gqevgeX6H6wKPM2drX-Q_X9-ldzatHF6meZ3h13fT9LNd7NPYVX9xs0t0lpisclf_tY3eJuPFaBaEL9PH0TAMSsoYDZLE0oQqnkAPYlCKMIikdEpxE1knetZGom-kk0ZJGlupeHMWFISDJFJUsDa6OeSWvvjYuKrWq2Lj8-alpoQprmSf84ZSB2qbZm6nS5-ujd9pAnovUe8l6qNEvRwOR8eJ_QKQ0mUT</recordid><startdate>20181130</startdate><enddate>20181130</enddate><creator>Werwein, Anton</creator><creator>Auer, Henry</creator><creator>Kuske, Lena</creator><creator>Kohlmann, Holger</creator><general>Wiley Subscription Services, Inc</general><scope/></search><sort><creationdate>20181130</creationdate><title>From Metallic LnTt (Ln = La, Nd; Tt = Si, Ge, Sn) to Electron‐precise Zintl Phase Hydrides LnTtH</title><author>Werwein, Anton ; Auer, Henry ; Kuske, Lena ; Kohlmann, Holger</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-p2332-ffc2f294f060d099130b77e994abce56ccb58a7e7a972dc794b775205e0fb9253</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2018</creationdate><topic>Conductors</topic><topic>DFT calculation</topic><topic>Electronic structure</topic><topic>Germanium</topic><topic>Hydrides</topic><topic>Hydrogen</topic><topic>Hydrogen atoms</topic><topic>Hydrogen storage</topic><topic>Hydrogenation</topic><topic>Lanthanides</topic><topic>Metal hydrides</topic><topic>Neodymium</topic><topic>Neutron diffraction</topic><topic>Quantum theory</topic><topic>Silicon compounds</topic><topic>Tin</topic><topic>Zintl phases</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Werwein, Anton</creatorcontrib><creatorcontrib>Auer, Henry</creatorcontrib><creatorcontrib>Kuske, Lena</creatorcontrib><creatorcontrib>Kohlmann, Holger</creatorcontrib><jtitle>Zeitschrift für anorganische und allgemeine Chemie (1950)</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Werwein, Anton</au><au>Auer, Henry</au><au>Kuske, Lena</au><au>Kohlmann, Holger</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>From Metallic LnTt (Ln = La, Nd; Tt = Si, Ge, Sn) to Electron‐precise Zintl Phase Hydrides LnTtH</atitle><jtitle>Zeitschrift für anorganische und allgemeine Chemie (1950)</jtitle><date>2018-11-30</date><risdate>2018</risdate><volume>644</volume><issue>22</issue><spage>1532</spage><epage>1539</epage><pages>1532-1539</pages><issn>0044-2313</issn><eissn>1521-3749</eissn><abstract>LnTt (Ln = La, Nd; Tt = Si, Ge, Sn) compounds crystallize in the CrB‐ or the FeB‐structure type with 1∞[Tt2–]‐polyanionic zigzag chains and can be rationalized as Ln3+Tt2–e–. They take up hydrogen at gas pressures from 10 to 160 bar and temperatures up to 750 K. The hydrides LnTtH1–x (0.04 ≤ x ≤ 0.39) crystallize either in a hydrogen filled CrB‐structure type (ZrNiH type, C‐phase, Cmcm: LaSiD0.92(1), LaGeD0.88(1), NdSiD, NdGeD0.95(1), LaSnHx) or in a hydrogen filled FeB‐structure type (LaGeH type, P‐phase, Pnma: LaSiD0.61(3), LaGeD0.96(4), NdSiD0.88(6)). In both cases, hydrogen atoms partially fill tetrahedral Ln4 voids as proven by neutron powder diffraction. While CrB‐structure type LnTt reacts to C‐phase only, FeB‐structure type LnTt hydrogenates to mixtures of C‐ (major phase) and P‐type hydrides. Electronic structure calculations reveal the depopulation of Ln‐d states, which cause the metallic conductivity in LnTt to be the main electronic effect upon hydrogenation. They further suggest Zintl phase hydrides LnTtH to be still poor metallic conductors with a pseudo bandgap at the Fermi level. The hydrogenation reaction from LnTt to LnTtH may thus be regarded as an incomplete metal to semiconductor transition.</abstract><cop>Weinheim</cop><pub>Wiley Subscription Services, Inc</pub><doi>10.1002/zaac.201800062</doi><tpages>8</tpages></addata></record> |
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subjects | Conductors DFT calculation Electronic structure Germanium Hydrides Hydrogen Hydrogen atoms Hydrogen storage Hydrogenation Lanthanides Metal hydrides Neodymium Neutron diffraction Quantum theory Silicon compounds Tin Zintl phases |
title | From Metallic LnTt (Ln = La, Nd; Tt = Si, Ge, Sn) to Electron‐precise Zintl Phase Hydrides LnTtH |
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