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Gold-Cage Perovskites: A Three-Dimensional Au III -X Framework Encasing Isolated MX 6 3- Octahedra (M III = In, Sb, Bi; X = Cl - , Br - , I - )
The Cs Au M X (M = In , Sb , Bi ; X = Cl , Br , I ) perovskites are composed of corner-sharing Au-X octahedra that trace the edges of a cube containing an isolated M-X octahedron at its body center. This structure, unique within the halide perovskite family, may be derived from the doubled cubic per...
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Published in: | Journal of the American Chemical Society 2021-05, Vol.143 (19), p.7440-7448 |
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creator | Lindquist, Kurt P Boles, Michael A Mack, Stephanie A Neaton, Jeffrey B Karunadasa, Hemamala I |
description | The Cs
Au
M
X
(M = In
, Sb
, Bi
; X = Cl
, Br
, I
) perovskites are composed of corner-sharing Au-X octahedra that trace the edges of a cube containing an isolated M-X octahedron at its body center. This structure, unique within the halide perovskite family, may be derived from the doubled cubic perovskite unit cell by removing the metals at the cube faces. To our knowledge, these are the only halide perovskites where the octahedral sites do not bear an average 2+ charge. Charge compensation in these materials requires a stoichiometric halide vacancy, which is disordered around the Au atom at the unit-cell corner and orders when the crystallization is slowed. Using X-ray crystallography, X-ray absorption spectroscopy, and pair distribution function analysis, we elucidate the structure of this unusual perovskite. Metal-site alloying produces further intricacies in this structure, which our model explains. Compared to other halide perovskites, this class of materials shows unusually low absorption onset energies ranging between ca. 1.0 and 2.4 eV. Partial reduction of Au
to Au
affords an intervalence charge-transfer band, which redshifts the absorption onset of Cs
Au
InCl
from 2.4 to 1.5 eV. With connected Au-X octahedra and isolated M-X octahedra, this structure type combines zero- and three-dimensional metal-halide sublattices in a single material and stands out among halide perovskites for its ordering of homovalent metals, ordering of halide vacancies, and incorporation of purely trivalent metals at the octahedral sites. |
doi_str_mv | 10.1021/jacs.1c01624 |
format | article |
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Au
M
X
(M = In
, Sb
, Bi
; X = Cl
, Br
, I
) perovskites are composed of corner-sharing Au-X octahedra that trace the edges of a cube containing an isolated M-X octahedron at its body center. This structure, unique within the halide perovskite family, may be derived from the doubled cubic perovskite unit cell by removing the metals at the cube faces. To our knowledge, these are the only halide perovskites where the octahedral sites do not bear an average 2+ charge. Charge compensation in these materials requires a stoichiometric halide vacancy, which is disordered around the Au atom at the unit-cell corner and orders when the crystallization is slowed. Using X-ray crystallography, X-ray absorption spectroscopy, and pair distribution function analysis, we elucidate the structure of this unusual perovskite. Metal-site alloying produces further intricacies in this structure, which our model explains. Compared to other halide perovskites, this class of materials shows unusually low absorption onset energies ranging between ca. 1.0 and 2.4 eV. Partial reduction of Au
to Au
affords an intervalence charge-transfer band, which redshifts the absorption onset of Cs
Au
InCl
from 2.4 to 1.5 eV. With connected Au-X octahedra and isolated M-X octahedra, this structure type combines zero- and three-dimensional metal-halide sublattices in a single material and stands out among halide perovskites for its ordering of homovalent metals, ordering of halide vacancies, and incorporation of purely trivalent metals at the octahedral sites.</description><identifier>ISSN: 0002-7863</identifier><identifier>EISSN: 1520-5126</identifier><identifier>DOI: 10.1021/jacs.1c01624</identifier><identifier>PMID: 33945275</identifier><language>eng</language><publisher>United States: American Chemical Society</publisher><ispartof>Journal of the American Chemical Society, 2021-05, Vol.143 (19), p.7440-7448</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c1305-34b87257d19e0d7be99f6773bbe94a99a5f89be6f7631ef91b67b750eb1aa71c3</citedby><cites>FETCH-LOGICAL-c1305-34b87257d19e0d7be99f6773bbe94a99a5f89be6f7631ef91b67b750eb1aa71c3</cites><orcidid>0000-0003-4949-8068 ; 0000000349498068</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.ncbi.nlm.nih.gov/pubmed/33945275$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink><backlink>$$Uhttps://www.osti.gov/biblio/1857564$$D View this record in Osti.gov$$Hfree_for_read</backlink></links><search><creatorcontrib>Lindquist, Kurt P</creatorcontrib><creatorcontrib>Boles, Michael A</creatorcontrib><creatorcontrib>Mack, Stephanie A</creatorcontrib><creatorcontrib>Neaton, Jeffrey B</creatorcontrib><creatorcontrib>Karunadasa, Hemamala I</creatorcontrib><title>Gold-Cage Perovskites: A Three-Dimensional Au III -X Framework Encasing Isolated MX 6 3- Octahedra (M III = In, Sb, Bi; X = Cl - , Br - , I - )</title><title>Journal of the American Chemical Society</title><addtitle>J Am Chem Soc</addtitle><description>The Cs
Au
M
X
(M = In
, Sb
, Bi
; X = Cl
, Br
, I
) perovskites are composed of corner-sharing Au-X octahedra that trace the edges of a cube containing an isolated M-X octahedron at its body center. This structure, unique within the halide perovskite family, may be derived from the doubled cubic perovskite unit cell by removing the metals at the cube faces. To our knowledge, these are the only halide perovskites where the octahedral sites do not bear an average 2+ charge. Charge compensation in these materials requires a stoichiometric halide vacancy, which is disordered around the Au atom at the unit-cell corner and orders when the crystallization is slowed. Using X-ray crystallography, X-ray absorption spectroscopy, and pair distribution function analysis, we elucidate the structure of this unusual perovskite. Metal-site alloying produces further intricacies in this structure, which our model explains. Compared to other halide perovskites, this class of materials shows unusually low absorption onset energies ranging between ca. 1.0 and 2.4 eV. Partial reduction of Au
to Au
affords an intervalence charge-transfer band, which redshifts the absorption onset of Cs
Au
InCl
from 2.4 to 1.5 eV. With connected Au-X octahedra and isolated M-X octahedra, this structure type combines zero- and three-dimensional metal-halide sublattices in a single material and stands out among halide perovskites for its ordering of homovalent metals, ordering of halide vacancies, and incorporation of purely trivalent metals at the octahedral sites.</description><issn>0002-7863</issn><issn>1520-5126</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2021</creationdate><recordtype>article</recordtype><recordid>eNo9kE1LxDAQhoMoun7cPMvgSWGjSdMkreJhXb8KioIKeytJOnWr3XZJquKv8C9bXfU088IzL8xDyDZnB5xF_PDZuHDAHeMqipfIgMuIUckjtUwGjLGI6kSJNbIewnMf4yjhq2RNiDSWkZYD8nnZ1gUdmyeEO_TtW3ipOgxHMIKHqUekZ9UMm1C1jalh9ApZlgGdwIU3M3xv_QucN86EqnmCLLS16bCAmwkoEBRuXWemWHgDezc_dyeQNUO4t0M4rY5h0udxDRT66H9G3wz7m2SlNHXArd-5QR4vzh_GV_T69jIbj66p44JJKmKb6EjqgqfICm0xTUultbD9Fps0NbJMUouq1EpwLFNulbZaMrTcGM2d2CC7i942dFUeXP-1m7q2adB1OU-kliruoeECcr4NwWOZz301M_4j5yz_lp9_y89_5ff4zgKfv9oZFv_wn23xBXaueI0</recordid><startdate>20210519</startdate><enddate>20210519</enddate><creator>Lindquist, Kurt P</creator><creator>Boles, Michael A</creator><creator>Mack, Stephanie A</creator><creator>Neaton, Jeffrey B</creator><creator>Karunadasa, Hemamala I</creator><general>American Chemical Society</general><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>OTOTI</scope><orcidid>https://orcid.org/0000-0003-4949-8068</orcidid><orcidid>https://orcid.org/0000000349498068</orcidid></search><sort><creationdate>20210519</creationdate><title>Gold-Cage Perovskites: A Three-Dimensional Au III -X Framework Encasing Isolated MX 6 3- Octahedra (M III = In, Sb, Bi; X = Cl - , Br - , I - )</title><author>Lindquist, Kurt P ; Boles, Michael A ; Mack, Stephanie A ; Neaton, Jeffrey B ; Karunadasa, Hemamala I</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c1305-34b87257d19e0d7be99f6773bbe94a99a5f89be6f7631ef91b67b750eb1aa71c3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2021</creationdate><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Lindquist, Kurt P</creatorcontrib><creatorcontrib>Boles, Michael A</creatorcontrib><creatorcontrib>Mack, Stephanie A</creatorcontrib><creatorcontrib>Neaton, Jeffrey B</creatorcontrib><creatorcontrib>Karunadasa, Hemamala I</creatorcontrib><collection>PubMed</collection><collection>CrossRef</collection><collection>OSTI.GOV</collection><jtitle>Journal of the American Chemical Society</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Lindquist, Kurt P</au><au>Boles, Michael A</au><au>Mack, Stephanie A</au><au>Neaton, Jeffrey B</au><au>Karunadasa, Hemamala I</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Gold-Cage Perovskites: A Three-Dimensional Au III -X Framework Encasing Isolated MX 6 3- Octahedra (M III = In, Sb, Bi; X = Cl - , Br - , I - )</atitle><jtitle>Journal of the American Chemical Society</jtitle><addtitle>J Am Chem Soc</addtitle><date>2021-05-19</date><risdate>2021</risdate><volume>143</volume><issue>19</issue><spage>7440</spage><epage>7448</epage><pages>7440-7448</pages><issn>0002-7863</issn><eissn>1520-5126</eissn><abstract>The Cs
Au
M
X
(M = In
, Sb
, Bi
; X = Cl
, Br
, I
) perovskites are composed of corner-sharing Au-X octahedra that trace the edges of a cube containing an isolated M-X octahedron at its body center. This structure, unique within the halide perovskite family, may be derived from the doubled cubic perovskite unit cell by removing the metals at the cube faces. To our knowledge, these are the only halide perovskites where the octahedral sites do not bear an average 2+ charge. Charge compensation in these materials requires a stoichiometric halide vacancy, which is disordered around the Au atom at the unit-cell corner and orders when the crystallization is slowed. Using X-ray crystallography, X-ray absorption spectroscopy, and pair distribution function analysis, we elucidate the structure of this unusual perovskite. Metal-site alloying produces further intricacies in this structure, which our model explains. Compared to other halide perovskites, this class of materials shows unusually low absorption onset energies ranging between ca. 1.0 and 2.4 eV. Partial reduction of Au
to Au
affords an intervalence charge-transfer band, which redshifts the absorption onset of Cs
Au
InCl
from 2.4 to 1.5 eV. With connected Au-X octahedra and isolated M-X octahedra, this structure type combines zero- and three-dimensional metal-halide sublattices in a single material and stands out among halide perovskites for its ordering of homovalent metals, ordering of halide vacancies, and incorporation of purely trivalent metals at the octahedral sites.</abstract><cop>United States</cop><pub>American Chemical Society</pub><pmid>33945275</pmid><doi>10.1021/jacs.1c01624</doi><tpages>9</tpages><orcidid>https://orcid.org/0000-0003-4949-8068</orcidid><orcidid>https://orcid.org/0000000349498068</orcidid></addata></record> |
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source | American Chemical Society:Jisc Collections:American Chemical Society Read & Publish Agreement 2022-2024 (Reading list) |
title | Gold-Cage Perovskites: A Three-Dimensional Au III -X Framework Encasing Isolated MX 6 3- Octahedra (M III = In, Sb, Bi; X = Cl - , Br - , I - ) |
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