Nanoscale Conical Swiss Roll with Broadband Visible and NIR Circular Dichroism
Source abstract
Abstract
A new strategy based on dynamic shadowing growth is developed to fabricate Swiss roll chiral metamaterials in nanoscale. The fabricated Swiss roll nanostructures exhibit broadband circular dichroism response in visible to near-IR wavelength region. Importantly, this strategy allows the dimension of Swiss rolls to be easily tuned, which subsequently changes their chiral optical properties. As a service to our authors and readers, this journal provides supporting information supplied by the authors. Such materials are peer reviewed and may be re-organized for online delivery, but are not copy-edited or typeset. Technical support issues arising from supporting information (other than missing files) should be addressed to the authors. Please note: The publisher is not responsible for the content or functionality of any supporting information supplied by the authors. Any queries (other than missing content) should be directed to the corresponding author for the article.
Source: openalex_inverted_index · Quality: baseline
Research context
OpenAlex topics: Metamaterials and Metasurfaces Applications · Plasmonic and Surface Plasmon Research · Liquid Crystal Research Advancements
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
Affiliations
Department of Physics and Astronomy and Nanoscale Science and Engineer Center University of Georgia Athens GA 30602 USA
Science and Technology on Plasma Physics Laboratory Research Center of Laser Fusion China Academy of Engineering Physics Mianyang 621900 P. R. China
References (36)
Show source-provided references
1. 10.1126/science.110446710.1126/science.1104467 ↗
2. 10.1088/0953-8984/21/37/37600310.1088/0953-8984/21/37/376003 ↗
3. 10.1016/j.physb.2010.01.00910.1016/j.physb.2010.01.009 ↗
4. 10.1126/science.109679610.1126/science.1096796 ↗
5. 10.1002/pssb.20067451110.1002/pssb.200674511 ↗
6. 10.1126/science.291.5505.84910.1126/science.291.5505.849 ↗
7. 10.1364/OE.11.00070910.1364/OE.11.000709 ↗
8. 10.1088/0953-8984/19/45/45621610.1088/0953-8984/19/45/456216 ↗
9. 10.1088/0953-8984/18/22/L0610.1088/0953-8984/18/22/L06 ↗
10. 10.1088/0953-8984/21/29/29220110.1088/0953-8984/21/29/292201 ↗
11. 10.1364/OL.32.00085610.1364/OL.32.000856 ↗
12. 10.1021/nl202565e10.1021/nl202565e ↗
13. 10.1021/nl300769x10.1021/nl300769x ↗
14. 10.1038/nature1088910.1038/nature10889 ↗
15. 10.1038/ncomms187710.1038/ncomms1877 ↗
16. 10.1021/nn402370x10.1021/nn402370x ↗
17. 10.1038/nmat368510.1038/nmat3685 ↗
18. 10.1021/nl403705k10.1021/nl403705k ↗
19. 10.1002/adma.20140229310.1002/adma.201402293 ↗
20. 10.1021/nl404572u10.1021/nl404572u ↗
21. 10.1021/nl403668710.1021/nl4036687 ↗
22. 10.1021/nl404823z10.1021/nl404823z ↗
23. 10.1002/adom.20130047810.1002/adom.201300478 ↗
24. 10.1103/PhysRevLett.102.16390310.1103/PhysRevLett.102.163903 ↗
25. 10.1103/PhysRevB.85.23530910.1103/PhysRevB.85.235309 ↗
26. 10.1063/1.470418510.1063/1.4704185 ↗
27. 10.1103/PhysRevB.79.08542910.1103/PhysRevB.79.085429 ↗
28. 10.1002/adma.20120057410.1002/adma.201200574 ↗
29. 10.1039/C4NR01878H10.1039/C4NR01878H ↗
30. 10.1002/adma.20100075510.1002/adma.201000755 ↗
31. 10.1039/C1SM06650A10.1039/C1SM06650A ↗
32. 10.1088/0957-4484/16/9/05210.1088/0957-4484/16/9/052 ↗
33. 10.1063/1.298889310.1063/1.2988893 ↗
34. 10.1088/2040-8978/15/7/07210110.1088/2040-8978/15/7/072101 ↗
35. 10.1021/nl402782d10.1021/nl402782d ↗
36. 10.1039/c3nr02666c10.1039/c3nr02666c ↗