Homogeneity range of ternary 11-type chalcogenides Fe1 + yTe1−xSex
dc.citation.epage | 2006 | en_US |
dc.citation.issueNumber | 7 | en_US |
dc.citation.spage | 2001 | en_US |
dc.citation.volumeNumber | 30 | en_US |
dc.contributor.author | Koz, C. | en_US |
dc.contributor.author | Rößler, S. | en_US |
dc.contributor.author | Wirth, S. | en_US |
dc.contributor.author | Schwarz, U. | en_US |
dc.date.accessioned | 2018-04-12T11:14:12Z | |
dc.date.available | 2018-04-12T11:14:12Z | |
dc.date.issued | 2017 | en_US |
dc.department | Institute of Materials Science and Nanotechnology (UNAM) | en_US |
dc.description.abstract | The 11-type Fe-chalcogenides belong to the family of Fe-based superconductors. In these compounds, the interstitial Fe is known to strongly influence the magnetic and superconducting properties. Here, we present the chemical homogeneity range of ternary compounds Fe1 + yTe1−xSex based on powder x-ray diffraction, energy dispersive x-ray analysis, and magnetization measurements. Our investigations show that the maximum amount of excess Fe in homogeneous Fe1 + yTe1−xSex decreases with increase in Se substitution for Te. Using our synthesis procedure, single-phase Fe1 + yTe1−xSex, with 0.5 ≤ x < 1 could not be formed for any amount of excess Fe. Further, the superconducting volume fraction in the material is found to be strongly suppressed by excess Fe. | en_US |
dc.description.provenance | Made available in DSpace on 2018-04-12T11:14:12Z (GMT). No. of bitstreams: 1 bilkent-research-paper.pdf: 179475 bytes, checksum: ea0bedeb05ac9ccfb983c327e155f0c2 (MD5) Previous issue date: 2017 | en |
dc.identifier.doi | 10.1007/s10948-016-3632-x | en_US |
dc.identifier.eissn | 1557-1947 | en_US |
dc.identifier.issn | 1557-1939 | |
dc.identifier.uri | http://hdl.handle.net/11693/37466 | |
dc.language.iso | English | en_US |
dc.publisher | Springer | en_US |
dc.relation.isversionof | http://dx.doi.org/10.1007/s10948-016-3632-x | en_US |
dc.source.title | Journal of Superconductivity and Novel Magnetism | en_US |
dc.subject | Fe-based superconductors | en_US |
dc.subject | Fe-chalcogenides | en_US |
dc.subject | Ternary phase diagram | en_US |
dc.subject | Chalcogenides | en_US |
dc.subject | Chemical analysis | en_US |
dc.subject | Chemical compounds | en_US |
dc.subject | Energy dispersive x-ray analysis | en_US |
dc.subject | Inorganic compounds | en_US |
dc.subject | Superconducting materials | en_US |
dc.subject | Ternary alloys | en_US |
dc.subject | X ray analysis | en_US |
dc.subject | X ray diffraction | en_US |
dc.subject | Chemical homogeneity | en_US |
dc.subject | Magnetization measurements | en_US |
dc.subject | Powder x-ray diffraction | en_US |
dc.subject | Superconducting properties | en_US |
dc.subject | Superconducting volume | en_US |
dc.subject | Synthesis procedure | en_US |
dc.subject | Iron compounds | en_US |
dc.title | Homogeneity range of ternary 11-type chalcogenides Fe1 + yTe1−xSex | en_US |
dc.type | Article | en_US |
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