Doping Evolution of the Superconducting Gap Structure in Heavily Hole-Doped Ba1-xKxFe2As2: a Heat Transport Study
We perform systematic thermal conductivity measurements on heavily hole-doped Ba1-xKxFe2As2 single crystals with 0.747 ≤ x ≤ 0.974. At x=0.747, the K0/T is negligible, indicating a nodeless superconducting gap. A small residual linear term K0/T (=0.035 m W.K-2 cm-1) appears at xz0.826, and it increa...
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description | We perform systematic thermal conductivity measurements on heavily hole-doped Ba1-xKxFe2As2 single crystals with 0.747 ≤ x ≤ 0.974. At x=0.747, the K0/T is negligible, indicating a nodeless superconducting gap. A small residual linear term K0/T (=0.035 m W.K-2 cm-1) appears at xz0.826, and it increases slowly up to x=0.974, followed by a substantial increase of more than 20 times to of K0/T clearly shows that the nodal gap appears near x surface topology. The small values of K0/T from x=0.826 the pure KFe2As2 (x=1.0). This doping dependence = 0.8, possibly associated with the change of Fermi to 0.974 are consistent with the Y-shaped nodal s- wave gap recently revealed by angle-resolved photoemission spectroscopy experiments at x=0.9. Furthermore, the substantial increase of K0/T from x=0.974 to 1.0 is inconsistent with a symmetry-imposed d-wave gap in KFe2 As2, and a possible nodal gap structure in KFe2As2 is discussed. |
doi_str_mv | 10.1088/0256-307X/32/12/127403 |
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At x=0.747, the K0/T is negligible, indicating a nodeless superconducting gap. A small residual linear term K0/T (=0.035 m W.K-2 cm-1) appears at xz0.826, and it increases slowly up to x=0.974, followed by a substantial increase of more than 20 times to of K0/T clearly shows that the nodal gap appears near x surface topology. The small values of K0/T from x=0.826 the pure KFe2As2 (x=1.0). This doping dependence = 0.8, possibly associated with the change of Fermi to 0.974 are consistent with the Y-shaped nodal s- wave gap recently revealed by angle-resolved photoemission spectroscopy experiments at x=0.9. Furthermore, the substantial increase of K0/T from x=0.974 to 1.0 is inconsistent with a symmetry-imposed d-wave gap in KFe2 As2, and a possible nodal gap structure in KFe2As2 is discussed.</description><identifier>ISSN: 0256-307X</identifier><identifier>EISSN: 1741-3540</identifier><identifier>DOI: 10.1088/0256-307X/32/12/127403</identifier><language>eng</language><subject>传热 ; 拓扑结构 ; 掺杂 ; 演变 ; 空穴 ; 能隙结构 ; 角分辨光电子能谱 ; 超导能隙</subject><ispartof>中国物理快报:英文版, 2015-12 (12), p.131-134</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Uhttp://image.cqvip.com/vip1000/qk/84212X/84212X.jpg</thumbnail><link.rule.ids>314,780,784,27924,27925</link.rule.ids></links><search><creatorcontrib>洪晓晨 王爱峰 张震 潘坚 何兰坡 罗习刚 陈仙辉 李世燕</creatorcontrib><title>Doping Evolution of the Superconducting Gap Structure in Heavily Hole-Doped Ba1-xKxFe2As2: a Heat Transport Study</title><title>中国物理快报:英文版</title><addtitle>Chinese Physics Letters</addtitle><description>We perform systematic thermal conductivity measurements on heavily hole-doped Ba1-xKxFe2As2 single crystals with 0.747 ≤ x ≤ 0.974. At x=0.747, the K0/T is negligible, indicating a nodeless superconducting gap. A small residual linear term K0/T (=0.035 m W.K-2 cm-1) appears at xz0.826, and it increases slowly up to x=0.974, followed by a substantial increase of more than 20 times to of K0/T clearly shows that the nodal gap appears near x surface topology. The small values of K0/T from x=0.826 the pure KFe2As2 (x=1.0). This doping dependence = 0.8, possibly associated with the change of Fermi to 0.974 are consistent with the Y-shaped nodal s- wave gap recently revealed by angle-resolved photoemission spectroscopy experiments at x=0.9. Furthermore, the substantial increase of K0/T from x=0.974 to 1.0 is inconsistent with a symmetry-imposed d-wave gap in KFe2 As2, and a possible nodal gap structure in KFe2As2 is discussed.</description><subject>传热</subject><subject>拓扑结构</subject><subject>掺杂</subject><subject>演变</subject><subject>空穴</subject><subject>能隙结构</subject><subject>角分辨光电子能谱</subject><subject>超导能隙</subject><issn>0256-307X</issn><issn>1741-3540</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2015</creationdate><recordtype>article</recordtype><recordid>eNo9j99KwzAUh4MoOKevIMH7uJwkbdLLOfdHFLzYBO9GlqZbpTY1Tcf2Kj6L7-QrmKIIh3P4cT4--CF0DfQWqFIjypKUcCpfR5yNoB8pKD9BA5ACCE8EPUWDf-gcXbTtG6UACmCA2nvXlPUWT_eu6kLpauwKHHYWL7vGeuPqvDOhB-a6wcvgY-q8xWWNF1bvy-qIF66yJFpsju80kMPjYWbZuGXfX59Y91TAK6_rtnE-REOXHy_RWaGr1l793SF6mU1XkwV5ep4_TMZPxIBigWiVKyEktSrRacFoKlWSWBCpUNRInbIs_ni2gQ2wLM9BaQ3ZpjAm7tgu40N08-s1O1dvP2KLdePLd-2P67SXqUQq_gMsSF35</recordid><startdate>20151201</startdate><enddate>20151201</enddate><creator>洪晓晨 王爱峰 张震 潘坚 何兰坡 罗习刚 陈仙辉 李世燕</creator><scope>2RA</scope><scope>92L</scope><scope>CQIGP</scope><scope>~WA</scope></search><sort><creationdate>20151201</creationdate><title>Doping Evolution of the Superconducting Gap Structure in Heavily Hole-Doped Ba1-xKxFe2As2: a Heat Transport Study</title><author>洪晓晨 王爱峰 张震 潘坚 何兰坡 罗习刚 陈仙辉 李世燕</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c182t-a8d84470e85a6f2067855e146480c7a62970e39b1b129dd18aa19bfcc19b11893</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2015</creationdate><topic>传热</topic><topic>拓扑结构</topic><topic>掺杂</topic><topic>演变</topic><topic>空穴</topic><topic>能隙结构</topic><topic>角分辨光电子能谱</topic><topic>超导能隙</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>洪晓晨 王爱峰 张震 潘坚 何兰坡 罗习刚 陈仙辉 李世燕</creatorcontrib><collection>中文科技期刊数据库</collection><collection>中文科技期刊数据库-CALIS站点</collection><collection>中文科技期刊数据库-7.0平台</collection><collection>中文科技期刊数据库- 镜像站点</collection><jtitle>中国物理快报:英文版</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>洪晓晨 王爱峰 张震 潘坚 何兰坡 罗习刚 陈仙辉 李世燕</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Doping Evolution of the Superconducting Gap Structure in Heavily Hole-Doped Ba1-xKxFe2As2: a Heat Transport Study</atitle><jtitle>中国物理快报:英文版</jtitle><addtitle>Chinese Physics Letters</addtitle><date>2015-12-01</date><risdate>2015</risdate><issue>12</issue><spage>131</spage><epage>134</epage><pages>131-134</pages><issn>0256-307X</issn><eissn>1741-3540</eissn><abstract>We perform systematic thermal conductivity measurements on heavily hole-doped Ba1-xKxFe2As2 single crystals with 0.747 ≤ x ≤ 0.974. At x=0.747, the K0/T is negligible, indicating a nodeless superconducting gap. A small residual linear term K0/T (=0.035 m W.K-2 cm-1) appears at xz0.826, and it increases slowly up to x=0.974, followed by a substantial increase of more than 20 times to of K0/T clearly shows that the nodal gap appears near x surface topology. The small values of K0/T from x=0.826 the pure KFe2As2 (x=1.0). This doping dependence = 0.8, possibly associated with the change of Fermi to 0.974 are consistent with the Y-shaped nodal s- wave gap recently revealed by angle-resolved photoemission spectroscopy experiments at x=0.9. Furthermore, the substantial increase of K0/T from x=0.974 to 1.0 is inconsistent with a symmetry-imposed d-wave gap in KFe2 As2, and a possible nodal gap structure in KFe2As2 is discussed.</abstract><doi>10.1088/0256-307X/32/12/127403</doi><tpages>4</tpages></addata></record> |
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source | IOP Publishing Journals; Institute of Physics (IOP) Journals - HEAL-Link; Alma/SFX Local Collection |
subjects | 传热 拓扑结构 掺杂 演变 空穴 能隙结构 角分辨光电子能谱 超导能隙 |
title | Doping Evolution of the Superconducting Gap Structure in Heavily Hole-Doped Ba1-xKxFe2As2: a Heat Transport Study |
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