Peculiar phase diagram with isolated superconducting regions in ThFeAsN1−xOx
ThFeAsN1−xOx () system with heavy electron doping has been studied by the measurements of x-ray diffraction, electrical resistivity, magnetic susceptibility and specific heat. The non-doped compound exhibits superconductivity at K, which is possibly due to an internal uniaxial chemical pressure that...
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creator | Li, Bai-Zhuo Wang, Zhi-Cheng Wang, Jia-Lu Zhang, Fu-Xiang Wang, Dong-Ze Zhang, Feng-Yuan Sun, Yu-Ping Jing, Qiang Zhang, Hua-Fu Tan, Shu-Gang Li, Yu-Ke Feng, Chun-Mu Mei, Yu-Xue Wang, Cao Cao, Guang-Han |
description | ThFeAsN1−xOx () system with heavy electron doping has been studied by the measurements of x-ray diffraction, electrical resistivity, magnetic susceptibility and specific heat. The non-doped compound exhibits superconductivity at K, which is possibly due to an internal uniaxial chemical pressure that is manifested by the extremely small value of As height with respect to the Fe plane. With the oxygen substitution, the Tc value decreases rapidly to below 2 K for , and surprisingly, superconductivity re-appears in the range of with a maximum of 17.5 K at x = 0.3. For the normal-state resistivity, while the samples in intermediate non-superconducting interval exhibit Fermi liquid behavior, those in other regions show a non-Fermi-liquid behavior. The specific heat jump for the superconducting sample of x = 0.4 is , which is discussed in terms of anisotropic superconducting gap. The peculiar phase diagram in ThFeAsN1−xOx presents additional ingredients for understanding the superconducting mechanism in iron-based superconductors. |
doi_str_mv | 10.1088/1361-648X/aac402 |
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The non-doped compound exhibits superconductivity at K, which is possibly due to an internal uniaxial chemical pressure that is manifested by the extremely small value of As height with respect to the Fe plane. With the oxygen substitution, the Tc value decreases rapidly to below 2 K for , and surprisingly, superconductivity re-appears in the range of with a maximum of 17.5 K at x = 0.3. For the normal-state resistivity, while the samples in intermediate non-superconducting interval exhibit Fermi liquid behavior, those in other regions show a non-Fermi-liquid behavior. The specific heat jump for the superconducting sample of x = 0.4 is , which is discussed in terms of anisotropic superconducting gap. The peculiar phase diagram in ThFeAsN1−xOx presents additional ingredients for understanding the superconducting mechanism in iron-based superconductors.</description><identifier>ISSN: 0953-8984</identifier><identifier>EISSN: 1361-648X</identifier><identifier>DOI: 10.1088/1361-648X/aac402</identifier><identifier>CODEN: JCOMEL</identifier><language>eng</language><publisher>IOP Publishing</publisher><subject>chemical pressure ; iron-based superconductors ; phase diagram</subject><ispartof>Journal of physics. Condensed matter, 2018-05, Vol.30 (25)</ispartof><rights>2018 IOP Publishing Ltd</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><orcidid>0000-0002-0870-9802 ; 0000-0001-9319-4737 ; 0000-0002-1330-0155</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://iopscience.iop.org/article/10.1088/1361-648X/aac402/pdf$$EPDF$$P50$$Giop$$H</linktopdf><link.rule.ids>314,776,780,27903,27904,53825,53872</link.rule.ids></links><search><creatorcontrib>Li, Bai-Zhuo</creatorcontrib><creatorcontrib>Wang, Zhi-Cheng</creatorcontrib><creatorcontrib>Wang, Jia-Lu</creatorcontrib><creatorcontrib>Zhang, Fu-Xiang</creatorcontrib><creatorcontrib>Wang, Dong-Ze</creatorcontrib><creatorcontrib>Zhang, Feng-Yuan</creatorcontrib><creatorcontrib>Sun, Yu-Ping</creatorcontrib><creatorcontrib>Jing, Qiang</creatorcontrib><creatorcontrib>Zhang, Hua-Fu</creatorcontrib><creatorcontrib>Tan, Shu-Gang</creatorcontrib><creatorcontrib>Li, Yu-Ke</creatorcontrib><creatorcontrib>Feng, Chun-Mu</creatorcontrib><creatorcontrib>Mei, Yu-Xue</creatorcontrib><creatorcontrib>Wang, Cao</creatorcontrib><creatorcontrib>Cao, Guang-Han</creatorcontrib><title>Peculiar phase diagram with isolated superconducting regions in ThFeAsN1−xOx</title><title>Journal of physics. Condensed matter</title><addtitle>JPhysCM</addtitle><addtitle>J. Phys.: Condens. Matter</addtitle><description>ThFeAsN1−xOx () system with heavy electron doping has been studied by the measurements of x-ray diffraction, electrical resistivity, magnetic susceptibility and specific heat. The non-doped compound exhibits superconductivity at K, which is possibly due to an internal uniaxial chemical pressure that is manifested by the extremely small value of As height with respect to the Fe plane. With the oxygen substitution, the Tc value decreases rapidly to below 2 K for , and surprisingly, superconductivity re-appears in the range of with a maximum of 17.5 K at x = 0.3. For the normal-state resistivity, while the samples in intermediate non-superconducting interval exhibit Fermi liquid behavior, those in other regions show a non-Fermi-liquid behavior. The specific heat jump for the superconducting sample of x = 0.4 is , which is discussed in terms of anisotropic superconducting gap. The peculiar phase diagram in ThFeAsN1−xOx presents additional ingredients for understanding the superconducting mechanism in iron-based superconductors.</description><subject>chemical pressure</subject><subject>iron-based superconductors</subject><subject>phase diagram</subject><issn>0953-8984</issn><issn>1361-648X</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2018</creationdate><recordtype>article</recordtype><sourceid/><recordid>eNptkM1KAzEUhYMoWKt7l9m5cWz-JsksS7EqlNZFBXfhNj9tSjszTGawj-DaR_RJ7FBxJVw4cPk4Bz6Ebil5oETrEeWSZlLo9xGAFYSdocHf6xwNSJHzTBdaXKKrlLaEEKG5GKD5q7fdLkKD6w0kj12EdQN7_BHbDY6p2kHrHU5d7Rtbla6zbSzXuPHrWJUJxxIvN1M_TnP6_fl1WByu0UWAXfI3vzlEb9PH5eQ5my2eXibjWRYZE20mpRMQCq9AWm8JpyxXihSKBC4Zz4NYWaZ8ICFXBYCzFiCsNJWEWe2UDHyI7k69sarNtuqa8rhm7N5wYlh-vPzImtr15P0_JCWmt2Z6RaZXZE7W-A9qAWGQ</recordid><startdate>20180525</startdate><enddate>20180525</enddate><creator>Li, Bai-Zhuo</creator><creator>Wang, Zhi-Cheng</creator><creator>Wang, Jia-Lu</creator><creator>Zhang, Fu-Xiang</creator><creator>Wang, Dong-Ze</creator><creator>Zhang, Feng-Yuan</creator><creator>Sun, Yu-Ping</creator><creator>Jing, Qiang</creator><creator>Zhang, Hua-Fu</creator><creator>Tan, Shu-Gang</creator><creator>Li, Yu-Ke</creator><creator>Feng, Chun-Mu</creator><creator>Mei, Yu-Xue</creator><creator>Wang, Cao</creator><creator>Cao, Guang-Han</creator><general>IOP Publishing</general><scope/><orcidid>https://orcid.org/0000-0002-0870-9802</orcidid><orcidid>https://orcid.org/0000-0001-9319-4737</orcidid><orcidid>https://orcid.org/0000-0002-1330-0155</orcidid></search><sort><creationdate>20180525</creationdate><title>Peculiar phase diagram with isolated superconducting regions in ThFeAsN1−xOx</title><author>Li, Bai-Zhuo ; Wang, Zhi-Cheng ; Wang, Jia-Lu ; Zhang, Fu-Xiang ; Wang, Dong-Ze ; Zhang, Feng-Yuan ; Sun, Yu-Ping ; Jing, Qiang ; Zhang, Hua-Fu ; Tan, Shu-Gang ; Li, Yu-Ke ; Feng, Chun-Mu ; Mei, Yu-Xue ; Wang, Cao ; Cao, Guang-Han</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-i224t-66d4af9e7a6cec03125770970f36235f4bc27ef0f579aadccaafb81602c8d76f3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2018</creationdate><topic>chemical pressure</topic><topic>iron-based superconductors</topic><topic>phase diagram</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Li, Bai-Zhuo</creatorcontrib><creatorcontrib>Wang, Zhi-Cheng</creatorcontrib><creatorcontrib>Wang, Jia-Lu</creatorcontrib><creatorcontrib>Zhang, Fu-Xiang</creatorcontrib><creatorcontrib>Wang, Dong-Ze</creatorcontrib><creatorcontrib>Zhang, Feng-Yuan</creatorcontrib><creatorcontrib>Sun, Yu-Ping</creatorcontrib><creatorcontrib>Jing, Qiang</creatorcontrib><creatorcontrib>Zhang, Hua-Fu</creatorcontrib><creatorcontrib>Tan, Shu-Gang</creatorcontrib><creatorcontrib>Li, Yu-Ke</creatorcontrib><creatorcontrib>Feng, Chun-Mu</creatorcontrib><creatorcontrib>Mei, Yu-Xue</creatorcontrib><creatorcontrib>Wang, Cao</creatorcontrib><creatorcontrib>Cao, Guang-Han</creatorcontrib><jtitle>Journal of physics. Condensed matter</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Li, Bai-Zhuo</au><au>Wang, Zhi-Cheng</au><au>Wang, Jia-Lu</au><au>Zhang, Fu-Xiang</au><au>Wang, Dong-Ze</au><au>Zhang, Feng-Yuan</au><au>Sun, Yu-Ping</au><au>Jing, Qiang</au><au>Zhang, Hua-Fu</au><au>Tan, Shu-Gang</au><au>Li, Yu-Ke</au><au>Feng, Chun-Mu</au><au>Mei, Yu-Xue</au><au>Wang, Cao</au><au>Cao, Guang-Han</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Peculiar phase diagram with isolated superconducting regions in ThFeAsN1−xOx</atitle><jtitle>Journal of physics. Condensed matter</jtitle><stitle>JPhysCM</stitle><addtitle>J. Phys.: Condens. Matter</addtitle><date>2018-05-25</date><risdate>2018</risdate><volume>30</volume><issue>25</issue><issn>0953-8984</issn><eissn>1361-648X</eissn><coden>JCOMEL</coden><abstract>ThFeAsN1−xOx () system with heavy electron doping has been studied by the measurements of x-ray diffraction, electrical resistivity, magnetic susceptibility and specific heat. The non-doped compound exhibits superconductivity at K, which is possibly due to an internal uniaxial chemical pressure that is manifested by the extremely small value of As height with respect to the Fe plane. With the oxygen substitution, the Tc value decreases rapidly to below 2 K for , and surprisingly, superconductivity re-appears in the range of with a maximum of 17.5 K at x = 0.3. For the normal-state resistivity, while the samples in intermediate non-superconducting interval exhibit Fermi liquid behavior, those in other regions show a non-Fermi-liquid behavior. The specific heat jump for the superconducting sample of x = 0.4 is , which is discussed in terms of anisotropic superconducting gap. The peculiar phase diagram in ThFeAsN1−xOx presents additional ingredients for understanding the superconducting mechanism in iron-based superconductors.</abstract><pub>IOP Publishing</pub><doi>10.1088/1361-648X/aac402</doi><tpages>7</tpages><orcidid>https://orcid.org/0000-0002-0870-9802</orcidid><orcidid>https://orcid.org/0000-0001-9319-4737</orcidid><orcidid>https://orcid.org/0000-0002-1330-0155</orcidid></addata></record> |
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title | Peculiar phase diagram with isolated superconducting regions in ThFeAsN1−xOx |
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