Subtle effect of doping on the charge density wave in TaTe2-delta (delta=0.028-0.123) crystals revealed by anisotropic transport measurements and Raman spectroscopy
Subtle effect of doping on the charge density wave in TaTe2-delta (delta=0.028-0.123) crystals revealed by anisotropic transport measurements and Raman spectroscopy
复制标题
各向异性输运测量和拉曼光谱揭示了掺杂对 TaTe2-delta (delta=0.028-0.123) 晶体中电荷密度波的微妙影响
DOI:
10.1103/physrevb.103.064103
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发表时间:
2021
影响因子:
3.7
通讯作者:
Chen Yan-Feng
中科院分区:
文献类型:
--
作者:
Luo Ye-Cheng;Lv Yang-Yang;Zhang Rui-Ming;Xu Lu;Zhu Zhi-An;Yao Shu-Hua;Zhou Jian;Xi Xiao-Xiang;Chen Y. B.;Chen Yan-Feng
The formation of charge density wave (CDW) is attributed to Fermi-surface nesting in textbooks, but this common paradigm is challenged by recent studies that reveal the pronounced effects of electron-phonon interaction and defects. Transition-metal dichalcogenide, being a prototype of charge density wave at around 170 K, is an ideal playground for exploring the mechanism of CDW. In this work, we reveal thesubtleeffect of defects on the CDW through studying a series of() crystals. Transport measurements show that, being close to the stoichiometric compound, have a resistivity-kink feature (fingerprint of CDW) around 160 K along both- andaxes;only has a resistivity-kink feature along theaxis. Remarkably, the resistivity kink completely disappears in. Raman spectroscopy not only confirms the corresponding structural phase transition, but also verifies decreased electron-phonon interaction at the Γ point of the Brillouin zone fromtobased on analysis of theoretical Fermi surface of 1phase ofbefore CDW phase transition. We propose that the CDW of() along theaxis is mainly due to electron-phonon interaction, while CDW along theaxis is the synergetic effect of Fermi-surface nesting and electron-phonon interaction; if dopant concentration is high enough, CDW is completely quenched by disorder induced by doping. Our study reveals the subtle effects of doping on CDW, and may give more hints on the interplay between CDW and high-temperature superconductor in the doped Mott insulators.