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Hall-plot of the phase diagram for Ba(Fe(1−x)Co(x))(2)As(2)

The Hall effect is a powerful tool for investigating carrier type and density. For single-band materials, the Hall coefficient is traditionally expressed simply by [Image: see text], where e is the charge of the carrier, and n is the concentration. However, it is well known that in the critical regi...

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Detalles Bibliográficos
Autores principales: Iida, Kazumasa, Grinenko, Vadim, Kurth, Fritz, Ichinose, Ataru, Tsukada, Ichiro, Ahrens, Eike, Pukenas, Aurimas, Chekhonin, Paul, Skrotzki, Werner, Teresiak, Angelika, Hühne, Ruben, Aswartham, Saicharan, Wurmehl, Sabine, Mönch, Ingolf, Erbe, Manuela, Hänisch, Jens, Holzapfel, Bernhard, Drechsler, Stefan-Ludwig, Efremov, Dmitri V.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group 2016
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4916655/
https://www.ncbi.nlm.nih.gov/pubmed/27328948
http://dx.doi.org/10.1038/srep28390
Descripción
Sumario:The Hall effect is a powerful tool for investigating carrier type and density. For single-band materials, the Hall coefficient is traditionally expressed simply by [Image: see text], where e is the charge of the carrier, and n is the concentration. However, it is well known that in the critical region near a quantum phase transition, as it was demonstrated for cuprates and heavy fermions, the Hall coefficient exhibits strong temperature and doping dependencies, which can not be described by such a simple expression, and the interpretation of the Hall coefficient for Fe-based superconductors is also problematic. Here, we investigate thin films of Ba(Fe(1−x)Co(x))(2)As(2) with compressive and tensile in-plane strain in a wide range of Co doping. Such in-plane strain changes the band structure of the compounds, resulting in various shifts of the whole phase diagram as a function of Co doping. We show that the resultant phase diagrams for different strain states can be mapped onto a single phase diagram with the Hall number. This universal plot is attributed to the critical fluctuations in multiband systems near the antiferromagnetic transition, which may suggest a direct link between magnetic and superconducting properties in the BaFe(2)As(2) system.