2020
DOI: 10.1209/0295-5075/130/67003
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The phase transition of ThFe1-xCoxAsN from superconductor to metallic paramagnet

Abstract: Differently from most of the other 1111-type iron-based superconductors, ThFeAsN itself shows superconductivity at 30 K without antiferromagnetism, even in the absence of chemical doping and other treating. In order to understand its peculiar behavior better, it is necessary to investigate the evolution of the superconducting phase through electron doping. Chemically, Co doping is a more effective way to introduce electrons, as carriers are doped directly into the FeAs planes. It also could provide information… Show more

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Cited by 7 publications
(1 citation statement)
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“…Similar to the LiFeAs superconductor, ThFeAsN has no structural phase instability, in contrast to the structural transition from the high-T tetragonal to low-T orthorhombic phase found in most of Fe-based superconductors [1]. Although strong magnetic fluctuations above 35 K have been reported [13], ThFeAsN shows unconventional superconductivity without antiferromagnetism, even in the absence of chemical doping and other treatings [11,14]. We recall here that band structure calculation predicts that undoped ThFeAsN should show stripe antiferromagnetic order similar to 1111 Fe-pnictides [15,16].…”
Section: Introductionmentioning
confidence: 89%
“…Similar to the LiFeAs superconductor, ThFeAsN has no structural phase instability, in contrast to the structural transition from the high-T tetragonal to low-T orthorhombic phase found in most of Fe-based superconductors [1]. Although strong magnetic fluctuations above 35 K have been reported [13], ThFeAsN shows unconventional superconductivity without antiferromagnetism, even in the absence of chemical doping and other treatings [11,14]. We recall here that band structure calculation predicts that undoped ThFeAsN should show stripe antiferromagnetic order similar to 1111 Fe-pnictides [15,16].…”
Section: Introductionmentioning
confidence: 89%