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Antiferromagnetic excitonic insulator state in Sr(3)Ir(2)O(7)

Excitonic insulators are usually considered to form via the condensation of a soft charge mode of bound electron-hole pairs. This, however, presumes that the soft exciton is of spin-singlet character. Early theoretical considerations have also predicted a very distinct scenario, in which the condens...

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Detalles Bibliográficos
Autores principales: Mazzone, D. G., Shen, Y., Suwa, H., Fabbris, G., Yang, J., Zhang, S.-S., Miao, H., Sears, J., Jia, Ke, Shi, Y. G., Upton, M. H., Casa, D. M., Liu, X., Liu, Jian, Batista, C. D., Dean, M. P. M.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group UK 2022
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8854623/
https://www.ncbi.nlm.nih.gov/pubmed/35177583
http://dx.doi.org/10.1038/s41467-022-28207-w
Descripción
Sumario:Excitonic insulators are usually considered to form via the condensation of a soft charge mode of bound electron-hole pairs. This, however, presumes that the soft exciton is of spin-singlet character. Early theoretical considerations have also predicted a very distinct scenario, in which the condensation of magnetic excitons results in an antiferromagnetic excitonic insulator state. Here we report resonant inelastic x-ray scattering (RIXS) measurements of Sr(3)Ir(2)O(7). By isolating the longitudinal component of the spectra, we identify a magnetic mode that is well-defined at the magnetic and structural Brillouin zone centers, but which merges with the electronic continuum in between these high symmetry points and which decays upon heating concurrent with a decrease in the material’s resistivity. We show that a bilayer Hubbard model, in which electron-hole pairs are bound by exchange interactions, consistently explains all the electronic and magnetic properties of Sr(3)Ir(2)O(7) indicating that this material is a realization of the long-predicted antiferromagnetic excitonic insulator phase.