Interface Engineering and Epitaxial Growth of Single‐Crystalline Aluminum Films on Semiconductors
Source abstract
Abstract
Abstract Single crystalline aluminum (Al) films are grown on GaAs substrates by molecular beam epitaxy. The high crystalline quality and sharp interfaces of the epitaxial Al films are confirmed by high‐resolution X‐ray diffraction and transmission electron microscopy. Semi‐metallic ErAs is inserted to the Al/GaAs interface to modify the band structure and reduce the optical loss of Al without degrading the crystalline quality. The optical dielectric properties of the Al films are measured by spectroscopic ellipsometry and the optical loss (ε2) is reduced in a broad spectral region from ultraviolet (UV) to near‐infrared compared to the widely quoted Palik's values. In particular, the loss in the visible region is reduced by a factor of three, indicating the effective energy band engineering by ErAs.
Source: crossref · Quality: baseline
Research context
OpenAlex topics: Semiconductor materials and devices · Optical Coatings and Gratings · GaN-based semiconductor devices and materials
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
Affiliations
National Laboratory of Solid State Microstructures and Department of Materials Science and Engineering College of Engineering and Applied Sciences Nanjing University Nanjing 210093 P. R. China
Jiangsu Key Laboratory of Artificial Functional Materials Nanjing 210093 P. R. China
Funding
National Basic Research Program of China · National Natural Science Foundation of China · Natural Science Foundation of Jiangsu Province · Fundamental Research Funds for the Central Universities
References (46)
Show source-provided references
1. 10.1126/science.111484910.1126/science.1114849 ↗
2. 10.1038/nphoton.2012.24410.1038/nphoton.2012.244 ↗
3. 10.1038/nature0193710.1038/nature01937 ↗
4. 10.1063/1.293073510.1063/1.2930735 ↗
5. 10.1038/nmat216210.1038/nmat2162 ↗
6. 10.1021/nn501379r10.1021/nn501379r ↗
7. 10.1038/nmat262910.1038/nmat2629 ↗
8. Huang C. · Appl. Phys. Lett. · 2012 · 100 · 893
9. 10.1103/PhysRev.128.162210.1103/PhysRev.128.1622 ↗
10. Olmon R. L. · Phys. Rev. B: Condens. Matter · 2015 · 86 · 278
11. 10.1103/PhysRevB.91.23513710.1103/PhysRevB.91.235137 ↗
12. 10.1126/science.119825810.1126/science.1198258 ↗
13. 10.1103/PhysRev.132.191810.1103/PhysRev.132.1918 ↗
14. 10.1021/nn405495q10.1021/nn405495q ↗
15. 10.1021/acsphotonics.7b0136610.1021/acsphotonics.7b01366 ↗
16. 10.1021/nn507088710.1021/nn5070887 ↗
17. 10.1038/nphoton.2013.23810.1038/nphoton.2013.238 ↗
18. 10.1021/acs.nanolett.6b0053710.1021/acs.nanolett.6b00537 ↗
19. 10.1038/ncomms595310.1038/ncomms5953 ↗
20. 10.1016/B978-0-08-054721-3.50018-610.1016/B978-0-08-054721-3.50018-6 ↗
21. 10.1021/acsnano.6b0555610.1021/acsnano.6b05556 ↗
22. 10.7567/JJAP.52.04580110.7567/JJAP.52.045801 ↗
23. 10.1016/j.actamat.2017.05.02610.1016/j.actamat.2017.05.026 ↗
24. 10.1038/srep1988710.1038/srep19887 ↗
25. Hao R. T. · J. Synth. Cryst. · 2014 · 43 · 1076
26. 10.1063/1.323717910.1063/1.3237179 ↗
27. 10.1088/0953-8984/28/40/40550110.1088/0953-8984/28/40/405501 ↗
28. 10.1088/1361-6528/aa578210.1088/1361-6528/aa5782 ↗
29. 10.1002/adma.20160517710.1002/adma.201605177 ↗
30. Klenov D. O. · Appl. Phys. Lett. · 2005 · 86 · 1631
31. 10.1021/nl401256310.1021/nl4012563 ↗
32. 10.1063/1.221320110.1063/1.2213201 ↗
33. 10.1557/PROC-221-8710.1557/PROC-221-87 ↗
34. 10.1116/1.359221110.1116/1.3592211 ↗
35. 10.1063/1.503394110.1063/1.5033941 ↗
36. 10.1016/j.mssp.2016.06.01110.1016/j.mssp.2016.06.011 ↗
37. Duan Q. · J. Synth. Cryst. · 2015 · 44 · 3467
38. 10.1080/0141861890822032810.1080/01418618908220328 ↗
39. 10.1134/S106378261503013610.1134/S1063782615030136 ↗
40. 10.1116/1.497120010.1116/1.4971200 ↗
41. 10.1103/PhysRevLett.107.03680610.1103/PhysRevLett.107.036806 ↗
42. 10.1002/adma.20140147410.1002/adma.201401474 ↗
43. 10.1016/S0040-6090(97)01001-810.1016/S0040-6090(97)01001-8 ↗
44. C. M.Herzinger B. D.Johs Dielectric Function Parametric Model and Method of Use1998 US5796983 A.
45. 10.1088/0022-3727/48/18/18400110.1088/0022-3727/48/18/184001 ↗
46. 10.1063/1.290821310.1063/1.2908213 ↗