Homogeneous superconducting gap in DyBa2Cu3O7-δ synthesized by oxide molecular beam epitaxy

被引:6
作者
Wu, Ze-Bin [1 ]
Putzky, Daniel [2 ]
Kundu, Asish K. [1 ]
Li, Hui [1 ,3 ]
Yang, Shize [1 ]
Du, Zengyi [1 ]
Joo, Sang Hyun [4 ]
Lee, Jinho [4 ]
Zhu, Yimei [1 ]
Logvenov, Gennady [1 ,2 ]
Keimer, Bernhard [2 ]
Fujita, Kazuhiro [1 ]
Valla, Tonica [1 ]
Bozovic, Ivan [1 ,5 ]
Drozdov, Ilya K. [1 ]
机构
[1] Brookhaven Natl Lab, Condensed Matter Phys & Mat Sci Div, Upton, NY 11973 USA
[2] Max Planck Inst Solid State Res, Heisenbergstr 1, D-70569 Stuttgart, Germany
[3] SUNY Stony Brook, Dept Phys & Astron, Stony Brook, NY 11794 USA
[4] Seoul Natl Univ, Dept Phys & Astron, Seoul 08826, South Korea
[5] Yale Univ, Dept Chem, New Haven, CT 06520 USA
来源
PHYSICAL REVIEW MATERIALS | 2020年 / 4卷 / 12期
基金
新加坡国家研究基金会;
关键词
HIGH-TEMPERATURE SUPERCONDUCTIVITY; COPPER OXIDES; PHASE-DIAGRAM; ENERGY-GAP; DENSITY; SURFACE; ORDER;
D O I
10.1103/PhysRevMaterials.4.124801
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
Much of what is known about high-temperature cuprate superconductors stems from studies based on two surface analytical tools, angle-resolved photoemission spectroscopy (ARPES) and spectroscopic imaging scanning tunneling microscopy (SI-STM). A question of general interest is whether and when the surface properties probed by ARPES and SI-STM are representative of the intrinsic properties of bulk materials. We find this question is prominent in thin films of a rarely studied cuprate DyBa2Cu3O7-delta (DBCO). We synthesize DBCO films by oxide molecular beam epitaxy and study them by in situ ARPES and SI-STM. Both ARPES and SI-STM show that the surface DBCO layer is different from the bulk of the film-it is heavily underdoped, while the doping level in the bulk is close to optimal doping evidenced by bulk-sensitive mutual inductance measurements. ARPES shows the typical electronic structure of a heavily underdoped CuO2 plane and two sets of one-dimensional bands originating from the CuO chains with one of them gapped. SI-STM reveals two different energy scales in the local density of states, with one (at similar to 18 meV) corresponding to the superconductivity and the other one (at similar to 90 meV) to the pseudogap. While the pseudogap shows large variations over the length scale of a few nanometers, the superconducting gap is very homogeneous. This indicates that the pseudogap and superconductivity are of different origins.
引用
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页数:9
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