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Unidirectional spin density wave state in metallic (Sr(1−x)La(x))(2)IrO(4)

Materials that exhibit both strong spin–orbit coupling and electron correlation effects are predicted to host numerous new electronic states. One prominent example is the J(eff) = 1/2 Mott state in Sr(2)IrO(4), where introducing carriers is predicted to manifest high temperature superconductivity an...

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Detalles Bibliográficos
Autores principales: Chen, Xiang, Schmehr, Julian L., Islam, Zahirul, Porter, Zach, Zoghlin, Eli, Finkelstein, Kenneth, Ruff, Jacob P. C., Wilson, Stephen D.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group UK 2018
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5760634/
https://www.ncbi.nlm.nih.gov/pubmed/29317642
http://dx.doi.org/10.1038/s41467-017-02647-1
Descripción
Sumario:Materials that exhibit both strong spin–orbit coupling and electron correlation effects are predicted to host numerous new electronic states. One prominent example is the J(eff) = 1/2 Mott state in Sr(2)IrO(4), where introducing carriers is predicted to manifest high temperature superconductivity analogous to the S = 1/2 Mott state of La(2)CuO(4). While bulk superconductivity currently remains elusive, anomalous quasiparticle behaviors paralleling those in the cuprates such as pseudogap formation and the formation of a d-wave gap are observed upon electron-doping Sr(2)IrO(4). Here we establish a magnetic parallel between electron-doped Sr(2)IrO(4) and hole-doped La(2)CuO(4) by unveiling a spin density wave state in electron-doped Sr(2)IrO(4). Our magnetic resonant X-ray scattering data reveal the presence of an incommensurate magnetic state reminiscent of the diagonal spin density wave state observed in the monolayer cuprate (La(1−x)Sr(x))(2)CuO(4). This link supports the conjecture that the quenched Mott phases in electron-doped Sr(2)IrO(4) and hole-doped La(2)CuO(4) support common competing electronic phases.