dc.contributor.author |
Prokes, K. |
en_US |
dc.contributor.author |
Matas, S. |
en_US |
dc.contributor.author |
HARNAGEA, LUMINITA |
en_US |
dc.contributor.author |
SINGH, S. |
en_US |
dc.contributor.author |
Wurmehl, S. |
en_US |
dc.contributor.author |
Argyriou, D.N. |
en_US |
dc.contributor.author |
Buechner, B. |
en_US |
dc.date.accessioned |
2019-02-14T05:49:51Z |
|
dc.date.available |
2019-02-14T05:49:51Z |
|
dc.date.issued |
2011-03 |
en_US |
dc.identifier.citation |
Physical Review B, 83(10), 104414 |
en_US |
dc.identifier.issn |
2469-9950 |
en_US |
dc.identifier.issn |
2469-9969 |
en_US |
dc.identifier.uri |
http://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/1786 |
|
dc.identifier.uri |
https://doi.org/10.1103/PhysRevB.83.104414 |
en_US |
dc.description.abstract |
Ca(Fe 1 − x Co x ) 2 As 2 single crystals with a concentration x = 0 . 032 , 0.039, 0.051, 0.056, and 0.063 were prepared and investigated by means of magnetic susceptibility and neutron diffraction combined with in situ electrical resistivity. The x - T phase diagram has been constructed. With increasing Co substitution, the anomaly marking the tetragonal to low-temperature orthorhombic structural phase transition temperature T S , the antiferromagnetic phase transition temperature T N , and the ordered magnetic moment gradually decrease. For samples with 0 . 039 ⩽ x ⩽ 0 . 056 , both transitions split and the T N appears at increasingly lower temperatures than T S . There is a small but finite difference between T S determined upon cooling and warming. For samples with x = 0 . 063 , no orthorhombic distortion and no long-range magnetic order is observed. For x ⩾ 0 . 051 superconductivity appears at low temperatures and the onset of the superconducting phase transition temperature T SC decreases slightly with increasing Co content. For the limited concentration range 0 . 051 ⩽ x ⩽ 0 . 056 , both long-range antiferromagnetism and superconductivity coexist. Comparison with Ba(Fe 1 − x Co x ) 2 As 2 indicates a more abrupt disappearance of magnetic order in Ca(Fe 1 − x Co x ) 2 As 2 . We find a direct correspondence between the magnitude of the ordered magnetic moment and the degree of orthorhombic splitting. |
en_US |
dc.language.iso |
en |
en_US |
dc.publisher |
American Physical Society |
en_US |
dc.subject |
Neutron diffraction |
en_US |
dc.subject |
Electrical resistivity |
en_US |
dc.subject |
Orthorhombic structural phase |
en_US |
dc.subject |
2011 |
en_US |
dc.title |
Effect of Co substitution on the magnetic order in Ca(Fe 1 − x Co x)2 As 2 single crystals studied by neutron diffraction |
en_US |
dc.type |
Article |
en_US |
dc.contributor.department |
Dept. of Physics |
en_US |
dc.identifier.sourcetitle |
Physical Review B |
en_US |
dc.publication.originofpublisher |
Foreign |
en_US |