Author
Listed:
- WEN-JUAN LI
(Institute of Physics, The Chinese Academy of Sciences, Beijing 100190, China)
- YU-JIE SUN
(Key Laboratory of Atomic and Nanosciences, Department of Physics, Tsinghua University, Beijing 100084, China)
- TONG ZHANG
(Institute of Physics, The Chinese Academy of Sciences, Beijing 100190, China)
- XIE-GANG ZHU
(Key Laboratory of Atomic and Nanosciences, Department of Physics, Tsinghua University, Beijing 100084, China)
- GUANG WANG
(Key Laboratory of Atomic and Nanosciences, Department of Physics, Tsinghua University, Beijing 100084, China)
- JIN-FENG JIA
(Key Laboratory of Atomic and Nanosciences, Department of Physics, Tsinghua University, Beijing 100084, China)
- XUCUN MA
(Institute of Physics, The Chinese Academy of Sciences, Beijing 100190, China)
- XI CHEN
(Key Laboratory of Atomic and Nanosciences, Department of Physics, Tsinghua University, Beijing 100084, China)
- QI-KUN XUE
(Institute of Physics, The Chinese Academy of Sciences, Beijing 100190, China;
Key Laboratory of Atomic and Nanosciences, Department of Physics, Tsinghua University, Beijing 100084, China)
Abstract
We have studied the superconductivity ofPbultra-thin films with thickness from 1 monolayer (ML) to 7 ML grown onSi(111)by molecular beam epitaxy.In situlow temperature scanning tunneling spectroscopy (STS) and angle-resolved photoemission spectroscopy (ARPES) measurements were performed on the films. It is suggested that the interface effect plays a critical role in enhancing the electron-phonon coupling, which consequently increases the superconducting transition temperature when a film reaches to the two-dimensional limit.
Suggested Citation
Wen-Juan Li & Yu-Jie Sun & Tong Zhang & Xie-Gang Zhu & Guang Wang & Jin-Feng Jia & Xucun Ma & Xi Chen & Qi-Kun Xue, 2010.
"ENHANCEMENT OF SUPERCONDUCTIVITY OFPbULTRA-THIN FILMS BY THE INTERFACE EFFECT,"
Surface Review and Letters (SRL), World Scientific Publishing Co. Pte. Ltd., vol. 17(04), pages 437-440.
Handle:
RePEc:wsi:srlxxx:v:17:y:2010:i:04:n:s0218625x10014235
DOI: 10.1142/S0218625X10014235
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