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Evolution of structure, magnetic and transport properties of Fe sub(1-x)Mn sub(x)Se

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dc.contributor.author Ingle, K.E.
dc.contributor.author Priolkar, K.R.
dc.contributor.author Bhobe, P.A.
dc.contributor.author Nigam, A.K.
dc.date.accessioned 2016-12-27T05:08:33Z
dc.date.available 2016-12-27T05:08:33Z
dc.date.issued 2016
dc.identifier.citation Materials Research Express. 3(12); 2016; Article ID 126001.
dc.identifier.uri http://dx.doi.org/10.1088/2053-1591/3/12/126001
dc.identifier.uri http://irgu.unigoa.ac.in/drs/handle/unigoa/4654
dc.description.abstract The present paper seeks to investigate effect of Mn doping in superconducting FeSe. It is found that over the entire doping range in Fe sub(1-x)Mn sub(x)Se ($0 less than or equal to xless than or equal to 1$), Mn does not substitute Fe in the superconducting tetragonal phase. Instead two impurity phases, NiAs type hexagonal phase and NaCl type cubic phase, grow with increasing Mn content. Initially, hexagonal phase has a higher content than the cubic phase but beyond x = 0.5, the cubic phase grows rapidly and for x greater than or equal to 0.8, the sample is monophasic with cubic NaCl type structure. The superconducting tetragonal phase content steadily decreases with increasing Mn concentration and completely disappears beyond x = 0.5. The premise that Mn never replaces Fe in the superconducting phase is further strengthened by observation of a sharp drop in AC susceptibility akin to superconducting transition at the T sub(c) of FeSe up to x = 0.5. EXAFS studies at the Fe K edge also show that the Fe has a four coordinated tetragonal local structure in all compositions below x = 0.5, similar to that in FeSe and it gradually changes to a six coordinated one as is expected for a NaCl type cubic phase for x greater than or equal to 0.5.
dc.publisher IOP Science
dc.subject Physics
dc.title Evolution of structure, magnetic and transport properties of Fe sub(1-x)Mn sub(x)Se
dc.type Journal article
dc.identifier.impf y


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