Systematic Doping Control of CVD Graphene Transistors with Functionalized Aromatic Self‐Assembled Monolayers
Source abstract
Abstract
Recent reports have shown that self‐assembled monolayers (SAMs) can induce doping effects in graphene transistors. However, a lack of understanding persists surrounding the quantitative relationship between SAM molecular design and its effects on graphene. In order to facilitate the fabrication of next‐generation graphene‐based devices it is important to reliably and predictably control the properties of graphene without negatively impacting its intrinsic high performance. In this study, SAMs with varying dipole magnitudes/directions are utilized and these values are directly correlated to changes in performance seen in graphene transistors. It is found that, by knowing the z‐component of the SAM dipole, one can reliably predict the shift in graphene charge neutrality point after taking into account the influence of the metal electrodes (which also play a role in doping graphene). This relationship is verified through density functional theory and comprehensive device studies utilizing atomic force microscopy, X‐ray photoelectron spectroscopy, Raman spectroscopy, and electrical characterization of graphene transistors. It is shown that properties of graphene transistors can be predictably controlled with SAMs when considering the total doping environment. Additionally, it is found that methylthio‐terminated SAMs strongly interact with graphene allowing for a cleaner graphene transfer and enhanced charge mobility.
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Research context
OpenAlex topics: Graphene research and applications · Molecular Junctions and Nanostructures · Quantum and electron transport phenomena
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
Affiliations
Department of Materials Science and Engineering, Box 352120 University of Washington Seattle WA 98195–2120 USA
Department of Physics, Box 351560 University of Washington Seattle WA 98195–1560 USA
Department of Chemistry, Box 351700 University of Washington Seattle WA 98195–1700 USA
References (68)
Show source-provided references
1. 10.1103/RevModPhys.81.10910.1103/RevModPhys.81.109 ↗
2. 10.1038/nature0423310.1038/nature04233 ↗
3. 10.1103/PhysRev.71.62210.1103/PhysRev.71.622 ↗
4. 10.1016/j.ssc.2008.02.02410.1016/j.ssc.2008.02.024 ↗
5. 10.1103/PhysRevLett.100.01660210.1103/PhysRevLett.100.016602 ↗
6. 10.1016/j.cplett.2009.06.00510.1016/j.cplett.2009.06.005 ↗
7. 10.1021/nn203377t10.1021/nn203377t ↗
8. 10.1021/nl200758b10.1021/nl200758b ↗
9. 10.1103/PhysRevB.86.04140910.1103/PhysRevB.86.041409 ↗
10. 10.1039/C0JM02922J10.1039/C0JM02922J ↗
11. 10.1002/adfm.20120099710.1002/adfm.201200997 ↗
12. 10.1021/nl303410g10.1021/nl303410g ↗
13. 10.1021/nn306012p10.1021/nn306012p ↗
14. 10.1021/nl803279t10.1021/nl803279t ↗
15. 10.1021/ja302483t10.1021/ja302483t ↗
16. 10.1021/nn300526210.1021/nn3005262 ↗
17. 10.1021/nl901572a10.1021/nl901572a ↗
18. 10.1103/PhysRevB.79.11540210.1103/PhysRevB.79.115402 ↗
19. 10.1103/PhysRevLett.101.02680310.1103/PhysRevLett.101.026803 ↗
20. 10.1103/PhysRevB.82.12110110.1103/PhysRevB.82.121101 ↗
21. 10.1021/nl201607t10.1021/nl201607t ↗
22. 10.1021/nn103484510.1021/nn1034845 ↗
23. 10.1021/jz200265w10.1021/jz200265w ↗
24. 10.1021/nn102236x10.1021/nn102236x ↗
25. 10.1002/adma.20040121610.1002/adma.200401216 ↗
26. 10.1063/1.290769110.1063/1.2907691 ↗
27. 10.1038/nature0337610.1038/nature03376 ↗
28. 10.1002/adfm.20110231210.1002/adfm.201102312 ↗
29. 10.1002/adfm.20090031510.1002/adfm.200900315 ↗
30. 10.1002/adma.20100150210.1002/adma.201001502 ↗
31. 10.1039/c0jm01292k10.1039/c0jm01292k ↗
32. 10.1063/1.368230110.1063/1.3682301 ↗
33. 10.1002/adma.20100476210.1002/adma.201004762 ↗
34. 10.1016/j.jcis.2004.12.00610.1016/j.jcis.2004.12.006 ↗
35. 10.1021/ja035956z10.1021/ja035956z ↗
36. 10.1039/b505422b10.1039/b505422b ↗
37. 10.1021/ja303807u10.1021/ja303807u ↗
38. 10.1103/PhysRev.136.B86410.1103/PhysRev.136.B864 ↗
39. 10.1103/PhysRev.140.A113310.1103/PhysRev.140.A1133 ↗
40. M. J.Frisch G. W.Trucks H. B.Schlegel G. E.Scuseria M. A.Robb J. R.Cheeseman G.Scalmani V.Barone B.Mennucci G. A.Petersson H.Nakatsuji M.Caricato X.Li H. P.Hratchian A. F.Izmaylov J.Bloino G.Zheng J. L.Sonnenberg M.Hada M.Ehara K.Toyota R.Fukuda J.Hasegawa M.Ishida T.Nakajima Y.Honda O.Kitao H.Nakai T.Vreven J. J. A.Montgomery J. E.Peralta F.Ogliaro M.Bearpark J. J.Heyd E.Brothers K. N.Kudin V. N.Staroverov R.Kobayashi J.Normand K.Raghavachari A.Rendell J. C.Burant S. S.Iyengar J.Tomasi M.Cossi N.Rega J. M.Millam M.Klene J. E.Knox J. B.Cross V.Bakken C.Adamo J.Jaramillo R.Gomperts R. E.Stratmann O.Yazyev A. J.Austin R.Cammi C.Pomelli J. W.Ochterski R. L.Martin K.Morokuma V. G.Zakrzewski G. A.Voth P.Salvador J. J.Dannenberg S.Dapprich A. D.Daniels Ö.Farkas J. B.Foresman J. V.Ortiz J.Cioslowski D. J.Fox Gaussian 09 Revision A.02 Gaussian Inc. Wallingford CT2009.
41. 10.1103/PhysRevLett.77.386510.1103/PhysRevLett.77.3865 ↗
42. 10.1063/1.46309610.1063/1.463096 ↗
43. 10.1016/0009-2614(95)00838-U10.1016/0009-2614(95)00838-U ↗
44. 10.1103/PhysRevB.20.39210.1103/PhysRevB.20.392 ↗
45. 10.1063/1.167410810.1063/1.1674108 ↗
46. 10.1103/PhysRevB.77.24540810.1103/PhysRevB.77.245408 ↗
47. 10.1103/PhysRevLett.97.18740110.1103/PhysRevLett.97.187401 ↗
48. 10.1016/S0368-2048(01)00310-310.1016/S0368-2048(01)00310-3 ↗
49. 10.1038/nnano.2010.13210.1038/nnano.2010.132 ↗
50. 10.1021/la052379e10.1021/la052379e ↗
51. 10.1016/S0167-5729(99)00002-310.1016/S0167-5729(99)00002-3 ↗
52. 10.1021/la304594t10.1021/la304594t ↗
53. 10.1021/jp064284710.1021/jp0642847 ↗
54. 10.1038/nmat246010.1038/nmat2460 ↗
55. 10.1039/c002639e10.1039/c002639e ↗
56. 10.1021/nl100504q10.1021/nl100504q ↗
57. 10.1088/0957-4484/23/27/27560510.1088/0957-4484/23/27/275605 ↗
58. 10.1002/smll.20110246810.1002/smll.201102468 ↗
59. 10.1038/nnano.2010.8910.1038/nnano.2010.89 ↗
60. 10.1021/nl102824h10.1021/nl102824h ↗
61. 10.1038/nmat184610.1038/nmat1846 ↗
62. 10.1038/nphys102210.1038/nphys1022 ↗
63. 10.1103/PhysRevB.79.19542510.1103/PhysRevB.79.195425 ↗
64. 10.1103/PhysRevB.81.08140810.1103/PhysRevB.81.081408 ↗
65. The Fermi level shift equation from reference 63 to determine the influence of Au metal doping on graphene was used:andThe parameter d represents the separation distance between the metal electrode and graphene with an equilibrium value determined to be 3.3 Å. The work function of Au (WM) was set as 5.25 eV whileWGrepresented the measured value of the graphene/SAM work function. Other parameters are standard parameters related to the graphene unit cell and are detailed further in reference 63.
66. In order to compensate for interaction/shielding effect between the underlying SAMs on graphene and the metal electrode work function it was assumed that the effective dipole was reduced and a correction factor was applied. For this factor WGfrom the equation in reference 65 was changed toWG0+b× ΔΦSAM. Where ΔΦSAMis the deviation from the untreated work function of graphene caused by the SAM and b is the correction factor equal to 0.679.WG0is the untreated work function of graphene measured to be 4.31 eV.
67. 10.1002/adma.20110341110.1002/adma.201103411 ↗
68. 10.1021/jz201098u10.1021/jz201098u ↗