4.8 Article

Electronic Structure Changes Due to Crystal Phase Switching at the Atomic Scale Limit

期刊

ACS NANO
卷 11, 期 10, 页码 10519-10528

出版社

AMER CHEMICAL SOC
DOI: 10.1021/acsnano.7b05873

关键词

nanowire; electronic structure; crystal phase; InAs; wurtzite; STM/S; zinc blende

资金

  1. Swedish Research Council (VR)
  2. Swedish Foundation for Strategic Research (SSF)
  3. Swedish energy agency
  4. Crafoord Foundation
  5. Knut and Alice Wallenberg Foundation
  6. European Research Council under the European Union's Seventh Framework Programme [259141]
  7. U.S. DOE Office of Science Facility [DE-SC0012704]

向作者/读者索取更多资源

The perfect switching between crystal phases with different electronic structure in III-V nanowires allows for the design of superstructures with quantum wells only a single atomic layer wide. However, it has only been indirectly inferred how the electronic structure will vary down to the smallest possible crystal segments. We use low-temperature scanning tunneling microscopy and spectroscopy to directly probe the electronic structure of Zinc blende (Zb) segments in Wurtzite (Wz) InAs nanowires with atomic-scale precision. We find that the major features in the band structure change abruptly down to a single atomic layer level. Distinct Zb electronic structure signatures are observed on both the conduction and valence band sides for the smallest possible Zb segment: a single InAs bilayer. We find evidence of confined states in the region of both single and double bilayer Zb segments indicative of the formation of crystal segment quantum wells due to the smaller band gap of Zb as compared to Wz. In contrast to the internal electronic structure of the nanowire, surface states located in the band gap were found to be only weakly influenced by the presence of the smallest Zb segments. Our findings directly demonstrate the feasibility of crystal phase switching for the ultimate limit of atomistic band structure engineering of quantum confined structures. Further, it indicates that band gap values obtained for the bulk are reasonable to use even for the smallest crystal segments. However, we also find that the suppression of surface and interface states could be necessary in the use of this effect for engineering of future electronic devices.

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