Ultracoherent Single‐Electron Emission of Carbon Nanotubes
Source abstract
Abstract
Abstract A single‐electron emitter, based on a single quantized energy level, can potentially achieve ultimate temporal and spatial coherence with a large emission current, which is desirable for atomic‐resolution electron probes. This is first developed by constructing a nano‐object on a metal tip to form a quantized double barrier structure. However, the single‐electron‐emission current can only achieve a picoampere level due to the low electron tunneling rate of the heterojunction with large barrier width, which limits the practical applications. In this study, carbon nanotubes (CNTs) serve as a single‐electron emitter and a current up to 1.5 nA is demonstrated. The double barrier structure formed on the CNT tip enables a high tunneling rate (≈1012 s−1) due to the smaller barrier width. The emitter also shows high temporal coherence (energy dispersion of ≈10 meV) and spatial coherence (effective source radius of ≈0.85 nm). This work represents a highly coherent electron source to simplify the electron optics system of atomic‐resolution electron microscopy and sub‐10 nm electron beam lithography.
Source: crossref · Quality: baseline
Research context
OpenAlex topics: Advanced Electron Microscopy Techniques and Applications · Force Microscopy Techniques and Applications · Carbon Nanotubes in Composites
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
Affiliations
CAS Key Laboratory of Nanophotonic Materials and Devices, CAS Key Laboratory of Standardization and Measurement for Nanotechnology, CAS Center for Excellence in Nanoscience National Center for Nanoscience and Technology Beijing 100190 P. R. China
Center of Materials Science and Optoelectronics Engineering University of Chinese Academy of Sciences Beijing 100049 P. R. China
Funding
National Natural Science Foundation of China
References (35)
Show source-provided references
1. 10.1016/j.ultramic.2019.04.00210.1016/j.ultramic.2019.04.002 ↗
2. 10.1016/S0304-3991(99)00034-010.1016/S0304-3991(99)00034-0 ↗
3. 10.1038/nature1387010.1038/nature13870 ↗
4. 10.1016/j.ultramic.2017.08.01610.1016/j.ultramic.2017.08.016 ↗
5. 10.1038/s41563-020-0763-z10.1038/s41563-020-0763-z ↗
6. 10.1093/jmicro/dfu02710.1093/jmicro/dfu027 ↗
7. 10.1103/PhysRevLett.74.470210.1103/PhysRevLett.74.4702 ↗
8. 10.1103/PhysRevB.47.1002010.1103/PhysRevB.47.10020 ↗
9. 10.1038/s41586-018-0223-y10.1038/s41586-018-0223-y ↗
10. 10.1103/PhysRevB.102.23543710.1103/PhysRevB.102.235437 ↗
11. 10.1103/PhysRevB.44.164610.1103/PhysRevB.44.1646 ↗
12. 10.1126/science.275.5308.192210.1126/science.275.5308.1922 ↗
13. 10.1073/pnas.091271610710.1073/pnas.0912716107 ↗
14. 10.1088/0034-4885/64/6/20110.1088/0034-4885/64/6/201 ↗
15. 10.1021/acsphotonics.0c0149010.1021/acsphotonics.0c01490 ↗
16. 10.1002/cvde.20050645210.1002/cvde.200506452 ↗
17. 10.1016/S0169-4332(99)00056-210.1016/S0169-4332(99)00056-2 ↗
18. 10.1103/PhysRevLett.112.12680510.1103/PhysRevLett.112.126805 ↗
19. 10.1021/jp021271u10.1021/jp021271u ↗
20. 10.1063/1.178663410.1063/1.1786634 ↗
21. 10.1021/jp810212g10.1021/jp810212g ↗
22. 10.1088/0957-4484/19/39/39570110.1088/0957-4484/19/39/395701 ↗
23. 10.1116/1.188007210.1116/1.1880072 ↗
24. 10.1126/science.115466310.1126/science.1154663 ↗
25. 10.1039/C4CS00231H10.1039/C4CS00231H ↗
26. 10.1103/PhysRevB.55.408110.1103/PhysRevB.55.4081 ↗
27. 10.1103/PhysRevB.77.20530810.1103/PhysRevB.77.205308 ↗
28. 10.1103/PhysRevB.73.11530510.1103/PhysRevB.73.115305 ↗
29. 10.1103/PhysRevLett.95.08680110.1103/PhysRevLett.95.086801 ↗
30. 10.1063/1.139631810.1063/1.1396318 ↗
31. 10.1063/5.003996110.1063/5.0039961 ↗
32. 10.1007/978-1-4939-6607-310.1007/978-1-4939-6607-3 ↗
33. 10.1103/PhysRevLett.114.10760110.1103/PhysRevLett.114.107601 ↗
34. 10.1021/acsphotonics.8b0041810.1021/acsphotonics.8b00418 ↗
35. 10.1103/PhysRevLett.114.22760110.1103/PhysRevLett.114.227601 ↗