Mapping Charge‐Carrier Density Across the p–n Junction in Ambipolar Carbon‐Nanotube Networks by Raman Microscopy
Source abstract
Abstract
In situ confocal Raman microscopy is used to map the recombination zone (induced p–n junction) in an ambipolar carbon-nanotube-network transistor with high spatial resolution. The shift of the 2D mode (G’ mode) depending on hole and electron accumulation serves as a measure for the local charge-carrier density and provides complementary information about charge transport and recombination in ambipolar transistors. 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: Carbon Nanotubes in Composites · Silicon Nanostructures and Photoluminescence · Nanopore and Nanochannel Transport Studies
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
Affiliations
Department of Materials Science and Engineering Friedrich‐Alexander‐Universität Erlangen‐Nürnberg 91058 Erlangen Germany
Universität Heidelberg Angewandte Physikalische Chemie 69120 Heidelberg Germany
References (46)
Show source-provided references
1. 10.1002/adma.20090371110.1002/adma.200903711 ↗
2. 10.1002/adfm.20090002810.1002/adfm.200900028 ↗
3. 10.1103/PhysRevB.73.20531610.1103/PhysRevB.73.205316 ↗
4. 10.1021/nn100966s10.1021/nn100966s ↗
5. 10.1021/nn403419d10.1021/nn403419d ↗
6. 10.1021/nl302389d10.1021/nl302389d ↗
7. 10.1021/nl202157510.1021/nl2021575 ↗
8. 10.1021/nl902062x10.1021/nl902062x ↗
9. 10.1002/adma.20120504110.1002/adma.201205041 ↗
10. 10.1021/nn200348p10.1021/nn200348p ↗
11. 10.1039/c3nr33723e10.1039/c3nr33723e ↗
12. 10.1002/adma.20130428010.1002/adma.201304280 ↗
13. 10.1002/adfm.20080189710.1002/adfm.200801897 ↗
14. 10.1063/1.289472310.1063/1.2894723 ↗
15. 10.1063/1.210600910.1063/1.2106009 ↗
16. 10.1002/cphc.20130001410.1002/cphc.201300014 ↗
17. 10.1063/1.296348810.1063/1.2963488 ↗
18. 10.1063/1.242902910.1063/1.2429029 ↗
19. 10.1002/adfm.20080086310.1002/adfm.200800863 ↗
20. 10.1002/adma.20100457210.1002/adma.201004572 ↗
21. 10.1002/adma.20110460210.1002/adma.201104602 ↗
22. 10.1126/science.125132910.1126/science.1251329 ↗
23. 10.1021/nn503046y10.1021/nn503046y ↗
24. 10.1016/j.orgel.2009.03.01010.1016/j.orgel.2009.03.010 ↗
25. 10.1143/JJAP.44.163310.1143/JJAP.44.1633 ↗
26. 10.1002/adma.20110241010.1002/adma.201102410 ↗
27. 10.1021/nn501118210.1021/nn5011182 ↗
28. 10.1002/adma.20140085910.1002/adma.201400859 ↗
29. 10.1038/nphoton.2007.17210.1038/nphoton.2007.172 ↗
30. 10.1038/nnano.2013.4610.1038/nnano.2013.46 ↗
31. Jorio A. · New J. Phys. · 2003 · 5 · 139110.1088/1367-2630/5/1/139 ↗
32. 10.1063/1.480391210.1063/1.4803912 ↗
33. 10.1021/nn203591j10.1021/nn203591j ↗
34. 10.1038/nnano.2007.32110.1038/nnano.2007.321 ↗
35. 10.1016/j.carbon.2009.10.03610.1016/j.carbon.2009.10.036 ↗
36. 10.1016/j.ssc.2013.05.01010.1016/j.ssc.2013.05.010 ↗
37. 10.1016/j.carbon.2008.08.02310.1016/j.carbon.2008.08.023 ↗
38. 10.1021/jp409849w10.1021/jp409849w ↗
39. 10.1002/adma.20120095010.1002/adma.201200950 ↗
40. 10.1038/nnano.2007.29010.1038/nnano.2007.290 ↗
41. 10.1021/nn305336x10.1021/nn305336x ↗
42. 10.1103/PhysRevB.78.24520210.1103/PhysRevB.78.245202 ↗
43. 10.1002/adfm.20120268910.1002/adfm.201202689 ↗
44. 10.1021/nn100331510.1021/nn1003315 ↗
45. 10.1021/ja210936n10.1021/ja210936n ↗
46. 10.1021/nl050378110.1021/nl0503781 ↗