22–27 Jul 2012
Embassy Suites Napa Valley
US/Pacific timezone

Three-Dimensional Electronic structure of Li1+xFeAs

23 Jul 2012, 20:00
2h
Fountain Court (Embassy Suites Napa Valley)

Fountain Court

Embassy Suites Napa Valley

1075 California Boulevard, Napa, California, United States 94559
Board: 32
Student Poster Competition Spin Phenomena Poster Session 1

Speaker

Tetsuya Hajiri (Nagoya University)

Description

Tetsuya Hajiri ^A, B^ Takahiro Ito ^A,C^ Ryosuke Niwa ^A^ Satoshi Hirate ^A^ Masaharu Matsunami ^B,D^ Byeong Hun Min ^E^, Yong Seung Kwon ^E^ Shin-ichi Kimura ^B,D^ ^A^ Graduate School of Engineering, Nagoya University, Nagoya 464-8603, Japan ^B^ UVSOR Facility, Institute for Molecular Science, Okazaki 444-8585, Japan ^C^ Nagoya University Synchrotron Radiation Research Center, Nagoya University, Nagoya, 464-8603, Japan ^D^ School of Physical Sciences, The Graduate University for Advanced Studies (SOKENDAI), Okazaki 444-8585, Japan ^E^ Department of Emerging Materials Science, DGIST, Daegu 711-873, Korea LiFeAs is an intriguing iron-based superconductor because it exhibits superconductivity (TC = 18 K) without any structural phase and SDW/AFM transitions [1]. In pristine LiFeAs, we have demonstrated that the electronic structure can be fundamentally explained by LDA band structure [2]. In this system, both of the excess and deficiency of Li-ions (Li1+xFeAs) from the stoichiometry suppresses the superconductivity [3] and enlarges spin fluctuation [4]. Up to date, the reason of the suppression of the superconductivity has not been clarified yet. To elucidate the effect of the Li excess or deficiency, we investigated the electronic structure of non-superconducting Li1+xFeAs by a polarization-dependent three-dimensional angle-resolved photoemission spectroscopy (3D-ARPES). As a result, we observed the difference in the low-energy electronic structure between pristine LiFeAs and Li1+xFeAs. We also found two kink structures in the band dispersions near the center of the Brillouin zone; one is located at about 20 meV, which originates from phonons, and the other at about 100 meV, which cannot be explained by the phonon origin. The higher-energy kink is considered to originate from magnetic excitations. [1] X. C. Wang et al., Solid State Commun. 148, 538-540 (2008). [2] T. Hajiri et al., to be published in Phys. Rev. B. [3] M. Wang et al., Phys. Rev. B 83, 220515(R) (2011). [4] L. Ma et al., Phys. Rev. B 82, 180501(R) (2010).

Primary author

Tetsuya Hajiri (Nagoya University)

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