Wafer‐Scale Patterning of Reduced Graphene Oxide Electrodes by Transfer‐and‐Reverse Stamping for High Performance OFETs
Source abstract
Abstract
Abstract A wafer‐scale patterning method for solution‐processed graphene electrodes, named the transfer‐and‐reverse stamping method, is universally applicable for fabricating source/drain electrodes of n‐ and p‐type organic field‐effect transistors with excellent performance. The patterning method begins with transferring a highly uniform reduced graphene oxide thin film, which is pre‐prepared on a glass substrate, onto hydrophobic silanized (rigid/flexible) substrates. Patterns of the as‐prepared reduced graphene oxide films are then formed by modulating the surface energy of the films and selectively delaminating the films using an oxygen‐plasma‐treated elastomeric stamp with patterns. Reduced graphene oxide patterns with various sizes and shapes can be readily formed onto an entire wafer. Also, they can serve as the source/drain electrodes for benchmark n‐ and p‐type organic field‐effect transistors with enhanced performance, compared to those using conventional metal electrodes. These results demonstrate the general utility of this technique. Furthermore, this simple, inexpensive, and scalable electrode‐patterning‐technique leads to assembling organic complementary circuits onto a flexible substrate successfully.
Source: crossref · Quality: baseline
Research context
OpenAlex topics: Nanowire Synthesis and Applications · Advanced Sensor and Energy Harvesting Materials · Organic Electronics and Photovoltaics
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
References (60)
Show source-provided references
1. 10.1038/4435910.1038/44359 ↗
2. 10.1002/(SICI)1521-4095(199803)10:5<365::AID-ADMA365>3.0.CO;2-U10.1002/(SICI)1521-4095(199803)10:5<365::AID-ADMA365>3.0.CO;2-U ↗
3. 10.1039/b411245h10.1039/b411245h ↗
4. 10.1002/adma.20030562310.1002/adma.200305623 ↗
5. 10.1039/b617995a10.1039/b617995a ↗
6. 10.1021/cm049647z10.1021/cm049647z ↗
7. 10.1002/adma.20100318810.1002/adma.201003188 ↗
8. 10.1016/j.orgel.2005.10.00210.1016/j.orgel.2005.10.002 ↗
9. 10.1021/am900483y10.1021/am900483y ↗
10. 10.1126/science.290.5499.212310.1126/science.290.5499.2123 ↗
11. 10.1063/1.294023210.1063/1.2940232 ↗
12. 10.1063/1.327386210.1063/1.3273862 ↗
13. 10.1063/1.271916210.1063/1.2719162 ↗
14. 10.1038/nmat229110.1038/nmat2291 ↗
15. 10.1002/adma.20050174010.1002/adma.200501740 ↗
16. 10.1021/ja045900k10.1021/ja045900k ↗
17. 10.1063/1.280623410.1063/1.2806234 ↗
18. 10.1002/adma.20080015010.1002/adma.200800150 ↗
19. 10.1002/adma.20080381210.1002/adma.200803812 ↗
20. 10.1002/adfm.20090040810.1002/adfm.200900408 ↗
21. 10.1021/nn100728p10.1021/nn100728p ↗
22. 10.1002/adma.20100416110.1002/adma.201004161 ↗
23. 10.1021/nl072838r10.1021/nl072838r ↗
24. 10.1038/nphoton.2011.31810.1038/nphoton.2011.318 ↗
25. 10.1002/adma.20100409910.1002/adma.201004099 ↗
26. 10.1021/nl902873610.1021/nl9028736 ↗
27. 10.1021/nl072090c10.1021/nl072090c ↗
28. 10.1039/B512799H10.1039/B512799H ↗
29. 10.1038/nnano.2008.8310.1038/nnano.2008.83 ↗
30. 10.1038/nnano.2007.45110.1038/nnano.2007.451 ↗
31. 10.1039/c2jm16232f10.1039/c2jm16232f ↗
32. 10.1002/adma.20100043610.1002/adma.201000436 ↗
33. 10.1021/nn100780v10.1021/nn100780v ↗
34. 10.1021/nn201118c10.1021/nn201118c ↗
35. 10.1002/adma.20110032910.1002/adma.201100329 ↗
36. 10.1002/adma.20080300010.1002/adma.200803000 ↗
37. 10.1039/C1JM14071J10.1039/C1JM14071J ↗
38. 10.1002/adma.20110034510.1002/adma.201100345 ↗
39. 10.1002/adfm.20110288810.1002/adfm.201102888 ↗
40. 10.1039/c2jm15299a10.1039/c2jm15299a ↗
41. 10.1021/ac980656z10.1021/ac980656z ↗
42. 10.1021/la100231u10.1021/la100231u ↗
43. 10.1080/0021846730807843710.1080/00218467308078437 ↗
44. 10.1002/adma.20060020610.1002/adma.200600206 ↗
45. The work of adhesion (WA12) between the layer 1 and 2 is calculated byWA12= 4(γ1dγ2d/(γ1d+γ2d) +γ1pγ2p/(γ1p+γ2p)) whereγdandγpare the dispersion and polar components of overall surface energy of a layer respectively. Those two contributions to the surface energy were obtained with two testing liquids water and ethylene glycol followed byγt(1 + cosθ) = 2(γtdγsd)1/2+ 2(γtpγsp)1/2 whereγtandγsdenote the surface energy of a testing liquid and a solid surface respectively andθis the contact angle.
46. 10.1002/adma.20030562310.1002/adma.200305623 ↗
47. 10.1002/marc.20050027610.1002/marc.200500276 ↗
48. 10.1002/adma.20080102410.1002/adma.200801024 ↗
49. 10.1063/1.153210210.1063/1.1532102 ↗
50. 10.1021/la063165f10.1021/la063165f ↗
51. 10.1063/1.156815710.1063/1.1568157 ↗
52. 10.1038/nature0337610.1038/nature03376 ↗
53. 10.1063/1.146770610.1063/1.1467706 ↗
54. 10.1039/b924415h10.1039/b924415h ↗
55. 10.1021/ja063290d10.1021/ja063290d ↗
56. 10.1021/cm071059910.1021/cm0710599 ↗
57. 10.1021/jp808037w10.1021/jp808037w ↗
58. 10.1039/c2jm31698f10.1039/c2jm31698f ↗
59. 10.1039/c1jm11607j10.1039/c1jm11607j ↗
60. 10.1021/ja01539a01710.1021/ja01539a017 ↗