Charge‐Generating Mode Control in High‐Performance Transparent Flexible Piezoelectric Nanogenerators
Source abstract
Abstract
Abstract In this work, we demonstrate the mode transition of charge generation between direct‐current (DC) and alternating‐current (AC) from transparent flexible (TF) piezoelectric nanogenerators (NGs), which is dependent solely on the morphology of zinc oxide (ZnO) nanorods without any use of an AC/DC converter. Tilted ZnO nanorods grown on a relatively low‐density seed layer generate DC‐type piezoelectric charges under a pushing load, whereas vertically aligned ZnO nanorods on a relatively high‐density seed layer create AC‐type charge generation. The mechanism for the geometry‐induced mode transition is proposed and characterized. We also examine the output performance of TF‐NGs which employ an indium zinc tin oxide (IZTO) film as a TF electrode. It is demonstrated that an IZTO film has improved electrical, optical, and mechanical properties, in comparison with an indium tin oxide (ITO) film. Enhanced output charge generation is observed from IZTO‐based TF‐NGs when TF‐NGs composed of only ITO electrodes are compared. This is attributed to the higher Schottky barrier and the lower series resistance of the IZTO‐based TF‐NGs. Thus, by using IZTO, we can expect TF‐NGs with superior mechanical durability and power generating performance.
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Research context
OpenAlex topics: Advanced Sensor and Energy Harvesting Materials · Conducting polymers and applications · Perovskite Materials and Applications
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
References (37)
Show source-provided references
1. 10.1021/ja810158x10.1021/ja810158x ↗
2. 10.1038/nnano.2008.1910.1038/nnano.2008.19 ↗
3. 10.1038/3510459910.1038/35104599 ↗
4. 10.1038/nature0618110.1038/nature06181 ↗
5. 10.1038/353073a010.1038/353073a0 ↗
6. 10.1038/nphoton.2009.6910.1038/nphoton.2009.69 ↗
7. 10.1038/3509801210.1038/35098012 ↗
8. 10.1126/science.113936610.1126/science.1139366 ↗
9. 10.1021/ja909863a10.1021/ja909863a ↗
10. 10.1126/science.114986010.1126/science.1149860 ↗
11. 10.1021/nl903377u10.1021/nl903377u ↗
12. 10.1002/adma.20090344210.1002/adma.200903442 ↗
13. 10.1021/nn900126k10.1021/nn900126k ↗
14. 10.1038/nature0660110.1038/nature06601 ↗
15. 10.1021/nl904071910.1021/nl9040719 ↗
16. 10.1021/nl061802g10.1021/nl061802g ↗
17. 10.1021/nl071256710.1021/nl0712567 ↗
18. Wang Z. L. · Adv. Func. Mater. · 2008 · 18 · 553
19. 10.1126/science.112400510.1126/science.1124005 ↗
20. 10.1002/adma.20060190810.1002/adma.200601908 ↗
21. Liu J. · Nano Lett. · 2008 · 8 · 28
22. 10.1504/IJNT.2007.01231310.1504/IJNT.2007.012313 ↗
23. 10.1021/nl803904b10.1021/nl803904b ↗
24. 10.1038/nnano.2010.4610.1038/nnano.2010.46 ↗
25. 10.1002/adma.20100116910.1002/adma.201001169 ↗
26. 10.1021/nn900523p10.1021/nn900523p ↗
27. 10.1002/adma.20080360510.1002/adma.200803605 ↗
28. 10.1021/jp909713c10.1021/jp909713c ↗
29. 10.1002/adma.20090381510.1002/adma.200903815 ↗
30. 10.1021/jp810814410.1021/jp8108144 ↗
31. 10.1016/j.jcrysgro.2007.02.01110.1016/j.jcrysgro.2007.02.011 ↗
32. 10.1007/s10854-007-9319-010.1007/s10854-007-9319-0 ↗
33. 10.1021/nl050788p10.1021/nl050788p ↗
34. Because the ZnO nanorod growth even on the high density seed layer can form tilted nanorods the pushing pressure can cause bending of the tilted ZnO nanorods. Thus we could obtain DC‐type output signals from V‐ZnO NGs but it was below 10%.
35. 10.1149/1.279974510.1149/1.2799745 ↗
36. 10.1063/1.293784510.1063/1.2937845 ↗
37. Jeong J.‐A. · J. Electrochem. Soc. · 2009 · 12 · J80