Emergence of Orbital Nematicity in the Tetragonal Phase of BaFe<sub>2</sub>(As<sub>1−</sub><i><sub>x</sub></i>P<i><sub>x</sub></i>)<sub>2</sub>
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- Tetsuya Iye
- Laboratoire National des Champs Magnétiques Intenses, LNCMI—CNRS (UPR3228), UJF, UPS and INSA, BP 166, 38042 Grenoble Cedex 9, France
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- Marc-Henri Julien
- Laboratoire National des Champs Magnétiques Intenses, LNCMI—CNRS (UPR3228), UJF, UPS and INSA, BP 166, 38042 Grenoble Cedex 9, France
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- Hadrien Mayaffre
- Laboratoire National des Champs Magnétiques Intenses, LNCMI—CNRS (UPR3228), UJF, UPS and INSA, BP 166, 38042 Grenoble Cedex 9, France
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- Mladen Horvatić
- Laboratoire National des Champs Magnétiques Intenses, LNCMI—CNRS (UPR3228), UJF, UPS and INSA, BP 166, 38042 Grenoble Cedex 9, France
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- Claude Berthier
- Laboratoire National des Champs Magnétiques Intenses, LNCMI—CNRS (UPR3228), UJF, UPS and INSA, BP 166, 38042 Grenoble Cedex 9, France
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- Kenji Ishida
- Department of Physics, Graduate School of Science, Kyoto University, Kyoto 606-8502, Japan
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- Hiroaki Ikeda
- Department of Physics, Graduate School of Science, Kyoto University, Kyoto 606-8502, Japan
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- Shigeru Kasahara
- Department of Physics, Graduate School of Science, Kyoto University, Kyoto 606-8502, Japan
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- Takasada Shibauchi
- Department of Physics, Graduate School of Science, Kyoto University, Kyoto 606-8502, Japan
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- Yuji Matsuda
- Department of Physics, Graduate School of Science, Kyoto University, Kyoto 606-8502, Japan
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説明
We report on $^{75}$As-NMR measurements in single crystalline BaFe$_{2}$(As$_{0.96}$P$_{0.04}$)$_{2}$ for magnetic fields parallel to the orthorhombic $[110]_{\rm o}$ and $[100]_{\rm o}$ directions above the structural transition temperature $T_{\rm S}\simeq121$ K. A large difference in the linewidth between the two field directions reveals in-plane anisotropy of the electric field gradient, even in the tetragonal phase. This provides microscopic evidence of population imbalance between As-$4p_{x}$ and $4p_{y}$ orbitals, which reaches $|n_x-n_y|/|n_x+n_y| \sim 15$\% at $T\rightarrow T_{\rm S}$ and is a natural consequence of the orbital ordering of Fe-3$d_{xz}$ and $d_{yz}$ electrons. Surprisingly, this orbital polarization is found to be already static near room temperature, suggesting that it arises from the pinning of anisotropic orbital fluctuations by disorder. The effect is found to be stronger below $\sim 160$ K, which coincides with the appearance of nematicity in previous torque and photoemission measurements. These results impose strong constraints on microscopic models of the nematic state.
6 pages, 6 figures. Supplemental Materials are included. To appear in J. Phys. Soc. Jpn. (Vol.84 No. 4)
収録刊行物
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- Journal of the Physical Society of Japan
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Journal of the Physical Society of Japan 84 (4), 043705-, 2015-04-15
Physical Society of Japan
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詳細情報 詳細情報について
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- CRID
- 1360565171311867392
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- NII論文ID
- 210000133500
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- ISSN
- 13474073
- 00319015
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- 資料種別
- journal article
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