In situ carrier tuning in high temperature superconductor Bi2Sr2CaCu2O(8+δ)by potassium deposition  被引量:1

In situ carrier tuning in high temperature superconductor Bi_2Sr_2CaCu_2O_(8+δ) by potassium deposition

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作  者:Yuxiao Zhang Cheng Hu Yong Hu Lin Zhao Ying Ding Xuan Sun Aiji Liang Yan Zhang Shaolong He Defa Liu Li Yu Guodong Liu Xiaoli Dong Genda Gu Chuangtian Chen Zuyan Xu Xingjiang Zhou 

机构地区:[1]National Laboratory for Superconductivity, Beijing National Laboratory for Condensed Matter Physics, Institute of Physics,Chinese Academy of Sciences, Beijing 100190, China [2]Brookhaven National Laboratory, Condensed Matter Physics and Materials Science Department, New York, NY 11973, USA [3]Technical Institute of Physics and Chemistry, Chinese Academy of Sciences, Beijing 100190, China [4]Collaborative Innovation Center of Quantum Matter,Beijing 100871, China

出  处:《Science Bulletin》2016年第13期1037-1043,共7页科学通报(英文版)

基  金:XJZ thanks financial support from the National Natural Science foundation of China (11190022,11334010 and 11534007);the National Basic Research Program of China (2015CB921000);the Strategic Priority Research Program (B) of Chinese Academy of Sciences (XDB07020300)

摘  要:We report a successful tuning of the hole doping level over a wide range in high temperature superconductor Bi2Sr2CaCu2O8+δ (Bi2212) through successive in situ potassium (K) deposition. By taking high resolution angleresolved photoemission measurements on the Fermi surface and band structure of an overdoped Bi2212 (To = 76 K) at different stages of K deposition, we found that the area of the hole-like Fermi surface around the Brillouin zone corner (n,n) shrinks with increasing K deposition. This indicates a continuous hole concentration change from initial - 0.26 to eventual 0.09 after extensive K deposition, a net doping level change of 0.17 that makes it possible to bring Bi2212 from being originally overdoped, to optimally-doped, and even- tually becoming heavily underdoped. The electronic behaviors with K deposition are consistent with those of Bi2212 samples with different hole doping levels. These results demonstrate that K deposition is an effective way of in situ controlling the hole concentration in Bi2212. This work opens a good way of studying the doping evolution of electronic structure and establishing the electronic phase diagram in Bi2212 that can be extended to other cuprate superconductors.We report a successful tuning of the hole doping level over a wide range in high temperature superconductor Bi_2Sr_2CaCu_2O_(8+δ)(Bi2212) through successive in situ potassium(K) deposition. By taking high resolution angleresolved photoemission measurements on the Fermi surface and band structure of an overdoped Bi2212(T_c= 76 K) at different stages of K deposition, we found that the area of the hole-like Fermi surface around the Brillouin zone corner(p,p) shrinks with increasing K deposition. This indicates a continuous hole concentration change from initial 0.26 to eventual 0.09 after extensive K deposition, a net doping level change of 0.17 that makes it possible to bring Bi2212 from being originally overdoped, to optimally-doped, and eventually becoming heavily underdoped. The electronic behaviors with K deposition are consistent with those of Bi2212 samples with different hole doping levels. These results demonstrate that K deposition is an effective way of in situ controlling the hole concentration in Bi2212. This work opens a good way of studying the doping evolution of electronic structure and establishing the electronic phase diagram in Bi2212 that can be extended to other cuprate superconductors.

关 键 词:Bi2212 - Superconductor- K-deposition -Photoemission Fermi surface 

分 类 号:TM26[一般工业技术—材料科学与工程]

 

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