Multiple-pseudogap phases in the hydrogen-doped LaFeAsO system

The low-energy electronic structure of LaFeAs⁢O1−⁢H (0.0≤≤0.60), a system which exhibits two superconducting domes and antiferromagnetic orders in its phase diagram, is investigated by utilizing laser photoemission spectroscopy. From the precise temperature-dependent measurement of the spectra near...

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Bibliographic Details
Main Author: Nakamura, A. (author)
Other Authors: Shimojima, T. (author), Sonobe, T. (author), Yoshida, S. (author), Ishizaka, K. (author), Malaeb, W. (author), Shin, S. (author), Iimura, S. (author), Matsuishi, S. (author)
Format: article
Published: 2017
Online Access:http://hdl.handle.net/10725/16704
https://doi.org/10.1103/PhysRevB.95.064501
http://libraries.lau.edu.lb/research/laur/terms-of-use/articles.php
https://journals.aps.org/prb/abstract/10.1103/PhysRevB.95.064501
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Summary:The low-energy electronic structure of LaFeAs⁢O1−⁢H (0.0≤≤0.60), a system which exhibits two superconducting domes and antiferromagnetic orders in its phase diagram, is investigated by utilizing laser photoemission spectroscopy. From the precise temperature-dependent measurement of the spectra near the Fermi level, we find a suppression of the density of states with cooling, namely a pseudogap formation, for all doping range. The pseudogap gets suppressed on doping through the first superconducting dome regime to the higher- region, whereas it tends to recover when further increasing toward the second antiferromagnetic ordered phase. The systematic doping dependence indicates the different origins of pseudogaps in the low- and high- regions, possibly related to the respective antiferromagnetic ground states residing at both ends of the phase diagram.