Plasmon‐Assisted Energy Transfer in Hybrid Nanosystems
Source abstract
Abstract
While direct optical excitation of carbon nanotubes activates only the tube species strictly matching the excitation source, excitation energy transfer processes provide a single excitation channel for all the nanotubes species in a sample. The requirement of an overlap between donor emission and acceptor absorption limits the poll of donors able to trasfer their excitation to the tubes, leaving the high‐energy part of the solar spectrum excluded from such processes. Here it is shown that the grafting of small metal nanoparticles to the tubes alters those rules, enabling energy transfer process from molecules for which the standard energy transfer process is strongly suppressed. The onset of an energy transfer band in the UV/blue spectral region is demonstrated for an hybrid gold‐pyrene‐nanotube system, yielding collective emission from all the tubes present in our samples upon excitation of pyrene.
Source: crossref · Quality: baseline
Research context
OpenAlex topics: Carbon Nanotubes in Composites · Gold and Silver Nanoparticles Synthesis and Applications · Nonlinear Optical Materials Studies
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
Affiliations
Department of Physics, Free University Berlin Arnimallee 14 14195 Berlin Germany
Department of Chemical Sciences, University of Padova via Marzolo 1 35131 Padova Italy
Funding
Deutsche Forschungsgemeinschaft
References (58)
Show source-provided references
1. 10.1038/nature0179710.1038/nature01797 ↗
2. 10.1126/science.111026510.1126/science.1110265 ↗
3. 10.1103/PhysRevB.72.24140210.1103/PhysRevB.72.241402 ↗
4. 10.1142/p08010.1142/p080 ↗
5. Reich S. · 2007
6. 10.1038/nnano.2015.13610.1038/nnano.2015.136 ↗
7. 10.1038/nphoton.2008.9410.1038/nphoton.2008.94 ↗
8. 10.1002/adfm.20160280310.1002/adfm.201602803 ↗
9. 10.1002/adma.20170671110.1002/adma.201706711 ↗
10. A nanotube species is uniquely identified by the so‐called chiral vector which specifies the length and direction of the nanotube folding expressed in the graphene unit vectors base.
11. 10.1126/science.107263110.1126/science.1072631 ↗
12. 10.1002/adfm.20120078410.1002/adfm.201200784 ↗
13. 10.1002/cphc.20100006710.1002/cphc.201000067 ↗
14. 10.1063/1.349647010.1063/1.3496470 ↗
15. 10.1063/1.481091210.1063/1.4810912 ↗
16. 10.1021/jp309818610.1021/jp3098186 ↗
17. 10.1002/pssb.20120019210.1002/pssb.201200192 ↗
18. 10.1021/nn302566e10.1021/nn302566e ↗
19. 10.1021/cm401312v10.1021/cm401312v ↗
20. 10.1039/C5NR08023A10.1039/C5NR08023A ↗
21. 10.1039/C6NR08942A10.1039/C6NR08942A ↗
22. 10.1088/1361-648X/aa824810.1088/1361-648X/aa8248 ↗
23. 10.1021/ja010172b10.1021/ja010172b ↗
24. 10.1021/es052208w10.1021/es052208w ↗
25. 10.1002/pssb.20100056010.1002/pssb.201000560 ↗
26. 10.1002/adfm.20110245110.1002/adfm.201102451 ↗
27. 10.1002/adma.20050149310.1002/adma.200501493 ↗
28. 10.1021/jz100940710.1021/jz1009407 ↗
29. 10.1021/ja107131r10.1021/ja107131r ↗
30. 10.1016/j.synthmet.2017.04.01810.1016/j.synthmet.2017.04.018 ↗
31. 10.1002/andp.1948437010510.1002/andp.19484370105 ↗
32. 10.1038/nphoton.2015.14210.1038/nphoton.2015.142 ↗
33. 10.1021/acs.jpclett.7b0052610.1021/acs.jpclett.7b00526 ↗
34. 10.1002/pssb.20170028110.1002/pssb.201700281 ↗
35. 10.1021/jp505005e10.1021/jp505005e ↗
36. 10.1016/j.cplett.2010.05.05210.1016/j.cplett.2010.05.052 ↗
37. 10.1002/cphc.20110069110.1002/cphc.201100691 ↗
38. 10.1021/cr03069810.1021/cr030698 ↗
39. 10.1103/PhysRev.93.9910.1103/PhysRev.93.99 ↗
40. 10.1016/j.physrep.2004.12.00210.1016/j.physrep.2004.12.002 ↗
41. 10.1103/PhysRevLett.102.07740110.1103/PhysRevLett.102.077401 ↗
42. 10.1103/PhysRevB.82.07542910.1103/PhysRevB.82.075429 ↗
43. 10.1364/OME.4.00258610.1364/OME.4.002586 ↗
44. 10.1063/1.497348010.1063/1.4973480 ↗
45. 10.1006/abio.1994.113410.1006/abio.1994.1134 ↗
46. In the case of ideal hertzian dipoles embedded in media with purely real dielectric constants those results simplify to the standard Förster case.[33]
47. 10.1021/nl803270x10.1021/nl803270x ↗
48. 10.1021/ar200331z10.1021/ar200331z ↗
49. 10.1038/ncomms1324010.1038/ncomms13240 ↗
50. 10.1088/0953-8984/24/39/39400510.1088/0953-8984/24/39/394005 ↗
51. 10.1088/0953-8984/24/39/39400610.1088/0953-8984/24/39/394006 ↗
52. 10.1080/1040663910804893310.1080/10406639108048933 ↗
53. 10.1021/bi300528510.1021/bi3005285 ↗
54. 10.1007/978-3-642-00710-110.1007/978-3-642-00710-1 ↗
55. 10.1002/bip.1977.36016101110.1002/bip.1977.360161011 ↗
56. 10.1007/s12274-013-0335-510.1007/s12274-013-0335-5 ↗
57. 10.1002/smll.20150388310.1002/smll.201503883 ↗
58. 10.1088/1361-6528/aa740910.1088/1361-6528/aa7409 ↗