Large zero bias peaks and dips in a four-terminal thin InAs-Al nanowire device
Large zero bias peaks and dips in a four-terminal thin InAs-Al nanowire device
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DOI:
10.1103/physrevresearch.4.033235
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发表时间:
2021-07
影响因子:
4.2
通讯作者:
Huading Song;Zitong Zhang;D. Pan;Dong E. Liu;Zhao-Jin Wang;Zhan-qiang Cao;Lei Liu;Lianjun Wen;Dunyuan Liao;Ran Zhuo;Dong E. Liu;Runan Shang;Jianhua Zhao;Haoqing Zhang
中科院分区:
文献类型:
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作者:
Huading Song;Zitong Zhang;D. Pan;Dong E. Liu;Zhao-Jin Wang;Zhan-qiang Cao;Lei Liu;Lianjun Wen;Dunyuan Liao;Ran Zhuo;Dong E. Liu;Runan Shang;Jianhua Zhao;Haoqing Zhang
We report electron transport studies of a thin InAs-Al hybrid semiconductor-superconductor nanowire device using a four-terminal design. Compared to previous works, thinner InAs nanowire (diameter less than 40 nm) is expected to reach fewer sub-band regime. The four-terminal device design excludes electrode contact resistance, an unknown value which has inevitably affected pre-viously reported device conductance. Using tunneling spectroscopy, we find large zero-bias peaks (ZBPs) in differential conductance on the order of 2 e 2 /h . Investigating the ZBP evolution by sweeping various gate voltages and magnetic field, we find a transition between a zero-bias peak and a zero-bias dip while the zero-bias conductance sticks close to 2 e 2 /h . We discuss a topologically trivial interpretation involving disorder, smooth potential variation and quasi-Majorana zero modes. Device Fabrication: The InAs nanowires were grown by molecular-beam epitaxy followed by an in-situ growth of Al film. The nanowires were then transferred from the growth chip to a p-doped Si/SiO 2 substrate by wipes of clean room tissues. Part of the Al film was selectively etched using Transene Aluminum Etchant Type D at 50 ◦ C for 10 seconds with etch windows patterned by electron-beam lithography (EBL). Electric contacts and side gates were fabricated in another round of EBL. Before metal deposition, a 40s long Argon plasma etching at a power of 50 W and pressure of 0.05 Torr was performed in the load-lock to ensure Ohmic contacts. Data Analysis: For all the 2D color maps of dI/dV vs V and B (or gate voltages), a bias offset V offset ( ∼ 50 uV) is estimated and subtracted from V , based on the symmetry of each data set which relies on the particle-hole symmetry of the superconducting gap (see data repository for V offset details). For the color-map plots, the dI/dV vs V curves are interpolated on to a regularly spaced V grid. Zero-bias line-cuts in bias scans are extracted based on the conductance value whose corresponding