In-Plane Anisotropic Response to Uniaxial Pressure in the Hidden Order State of URu2Si2
We investigate the uniaxial-pressure dependence of resistivity for URu2-xFexSi2 samples with x=0 and 0.2,which host a hidden order(HO)and a large-moment antiferromagnetic(LMAFM)phase,respectively.For both samples,the elastoresistivity ζ shows a seemingly divergent behavior above the transition tempe...
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Abstract | We investigate the uniaxial-pressure dependence of resistivity for URu2-xFexSi2 samples with x=0 and 0.2,which host a hidden order(HO)and a large-moment antiferromagnetic(LMAFM)phase,respectively.For both samples,the elastoresistivity ζ shows a seemingly divergent behavior above the transition temperature To and a quick decrease below it.We find that the temperature dependence of ζ for both samples can be well described by assuming the uniaxial pressure effect on the gap or certain energy scale except for ζ(110)of the x=0 sample,which exhibits a nonzero residual value at 0 K.We show that this provides a qualitative difference between the HO and LMAFM phases.Our results suggest that there is an in-plane anisotropic response to the uniaxial pressure that only exists in the hidden order state without necessarily breaking the rotational lattice symmetry. |
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AbstractList | We investigate the uniaxial-pressure dependence of resistivity for URu2-xFexSi2 samples with x=0 and 0.2,which host a hidden order(HO)and a large-moment antiferromagnetic(LMAFM)phase,respectively.For both samples,the elastoresistivity ζ shows a seemingly divergent behavior above the transition temperature To and a quick decrease below it.We find that the temperature dependence of ζ for both samples can be well described by assuming the uniaxial pressure effect on the gap or certain energy scale except for ζ(110)of the x=0 sample,which exhibits a nonzero residual value at 0 K.We show that this provides a qualitative difference between the HO and LMAFM phases.Our results suggest that there is an in-plane anisotropic response to the uniaxial pressure that only exists in the hidden order state without necessarily breaking the rotational lattice symmetry. |
Author | Wang, Xingyu Zhao, Jinyu Tan, Shiyong Lai, Xinchun Li, Shiliang Sheng, Yutao Gong, Dongliang Liu, Bo Sun, Liling Yang, Yi-feng Ma, Xiaoyan Zhang, Wen Wang, Pengyu Guo, Jing |
AuthorAffiliation | Beijing National Laboratory for Condensed Matter Physics,Institute of Physics,Chinese Academy of Sciences,Beijing 100190,China;School of Physical Sciences,University of Chinese Academy of Sciences,Beijing 100190,China%Beijing National Laboratory for Condensed Matter Physics,Institute of Physics,Chinese Academy of Sciences,Beijing 100190,China%Beijing National Laboratory for Condensed Matter Physics,Institute of Physics,Chinese Academy of Sciences,Beijing 100190,China;Songshan Lake Materials Laboratory,Dongguan 523808,China%Beijing National Laboratory for Condensed Matter Physics,Institute of Physics,Chinese Academy of Sciences,Beijing 100190,China;School of Physical Sciences,University of Chinese Academy of Sciences,Beijing 100190,China;Songshan Lake Materials Laboratory,Dongguan 523808,China%State Key Laboratory of Environment-friendly Energy Materials,Southwest University of Science and Technology,Mianyang 621010,China;Science and Technology on Surface Physics and Chemistry Laborator |
AuthorAffiliation_xml | – name: Beijing National Laboratory for Condensed Matter Physics,Institute of Physics,Chinese Academy of Sciences,Beijing 100190,China;School of Physical Sciences,University of Chinese Academy of Sciences,Beijing 100190,China%Beijing National Laboratory for Condensed Matter Physics,Institute of Physics,Chinese Academy of Sciences,Beijing 100190,China%Beijing National Laboratory for Condensed Matter Physics,Institute of Physics,Chinese Academy of Sciences,Beijing 100190,China;Songshan Lake Materials Laboratory,Dongguan 523808,China%Beijing National Laboratory for Condensed Matter Physics,Institute of Physics,Chinese Academy of Sciences,Beijing 100190,China;School of Physical Sciences,University of Chinese Academy of Sciences,Beijing 100190,China;Songshan Lake Materials Laboratory,Dongguan 523808,China%State Key Laboratory of Environment-friendly Energy Materials,Southwest University of Science and Technology,Mianyang 621010,China;Science and Technology on Surface Physics and Chemistry Laboratory,Mianyang 621908,China%Science and Technology on Surface Physics and Chemistry Laboratory,Mianyang 621908,China |
Author_xml | – sequence: 1 givenname: Xingyu surname: Wang fullname: Wang, Xingyu organization: School of Physical Sciences, University of Chinese Academy of Sciences , China – sequence: 2 givenname: Dongliang surname: Gong fullname: Gong, Dongliang organization: Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences , China – sequence: 3 givenname: Bo surname: Liu fullname: Liu, Bo organization: School of Physical Sciences, University of Chinese Academy of Sciences , China – sequence: 4 givenname: Xiaoyan surname: Ma fullname: Ma, Xiaoyan organization: School of Physical Sciences, University of Chinese Academy of Sciences , China – sequence: 5 givenname: Jinyu surname: Zhao fullname: Zhao, Jinyu organization: School of Physical Sciences, University of Chinese Academy of Sciences , China – sequence: 6 givenname: Pengyu surname: Wang fullname: Wang, Pengyu organization: School of Physical Sciences, University of Chinese Academy of Sciences , China – sequence: 7 givenname: Yutao surname: Sheng fullname: Sheng, Yutao organization: School of Physical Sciences, University of Chinese Academy of Sciences , China – sequence: 8 givenname: Jing surname: Guo fullname: Guo, Jing organization: Songshan Lake Materials Laboratory , China – sequence: 9 givenname: Liling surname: Sun fullname: Sun, Liling organization: Songshan Lake Materials Laboratory , China – sequence: 10 givenname: Wen surname: Zhang fullname: Zhang, Wen organization: Science and Technology on Surface Physics and Chemistry Laboratory , China – sequence: 11 givenname: Xinchun surname: Lai fullname: Lai, Xinchun organization: Science and Technology on Surface Physics and Chemistry Laboratory , China – sequence: 12 givenname: Shiyong surname: Tan fullname: Tan, Shiyong organization: Science and Technology on Surface Physics and Chemistry Laboratory , China – sequence: 13 givenname: Yi-feng surname: Yang fullname: Yang, Yi-feng organization: Songshan Lake Materials Laboratory , China – sequence: 14 givenname: Shiliang surname: Li fullname: Li, Shiliang organization: Songshan Lake Materials Laboratory , China |
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Snippet | We investigate the uniaxial-pressure dependence of resistivity for URu2-xFexSi2 samples with x=0 and 0.2,which host a hidden order(HO)and a large-moment... |
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Title | In-Plane Anisotropic Response to Uniaxial Pressure in the Hidden Order State of URu2Si2 |
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