journal article·2012-03-07Open access

Structure and Morphology of PDI8‐CN2 for n‐Type Thin‐Film Transistors

Fabiola Liscio, Silvia Milita, Cristiano Albonetti, Pasquale D'Angelo, Antonietta Guagliardi, Norberto Masciocchi, Raffaele Guido Della Valle, Elisabetta Venuti, Aldo Brillante, Fabio Biscarini

Advanced Functional Materials· Volume 22· Issue 5

Abstract

Abstract A multiscale investigation of N,N′‐bis(n‐octyl)‐x:y, dicyanoperylene‐3,4:9,10‐bis(dicarboximide), PDI8‐CN2, shows the same molecular arrangement in the bulk and in thin films sublimated on SiO2/Si wafers. Non‐conventional powder diffraction methods and theoretical calculations concur to provide a coherent picture of the crystalline structure. X‐ray diffraction (XRD) and atomic force microscopy (AFM) analyses of films of different thickness deposited at different substrate temperatures indicate the existence of two temperature‐dependent deposition regimes: a low‐temperature (room temperature) regime and a high‐temperature (80–120 °C) one, each characterized by different growth mechanisms. These mechanisms eventually result in different morphological and structural features of the films, which appear to be highly correlated with the trend of the electrical parameters that are measured in PDI8‐CN2‐based field‐effect transistors.
Source: crossref · Quality: baseline

Research context

OpenAlex topics: Advanced Memory and Neural Computing · Organic Electronics and Photovoltaics · Semiconductor materials and devices

SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.

References (100+)

Show source-provided references
1. 10.1002/1521-4095(20020116)14:2<99::AID-ADMA99>3.0.CO;2-910.1002/1521-4095(20020116)14:2<99::AID-ADMA99>3.0.CO;2-9 ↗
2. 10.1038/nature0249810.1038/nature02498 ↗
3. 10.1038/nature0298710.1038/nature02987 ↗
4. 10.1126/science.114645810.1126/science.1146458 ↗
5. 10.1038/nnano.2007.36510.1038/nnano.2007.365 ↗
6. 10.1038/nmat205910.1038/nmat2059 ↗
7. 10.1038/nmat229110.1038/nmat2291 ↗
8. 10.1038/nmat212210.1038/nmat2122 ↗
9. 10.1021/nl103200r10.1021/nl103200r ↗
10. 10.1073/pnas.09158809810.1073/pnas.091588098 ↗
11. 10.1038/nmat106110.1038/nmat1061 ↗
12. 10.1126/science.120305210.1126/science.1203052 ↗
13. 10.1126/science.270.5238.97210.1126/science.270.5238.972 ↗
14. 10.1063/1.136078510.1063/1.1360785 ↗
15. 10.1038/nmat76810.1038/nmat768 ↗
16. 10.1073/pnas.051075010310.1073/pnas.0510750103 ↗
17. 10.1073/pnas.080210510510.1073/pnas.0802105105 ↗
18. 10.1038/3500053010.1038/35000530 ↗
19. 10.1002/adma.20050267710.1002/adma.200502677 ↗
20. 10.1038/nature0553310.1038/nature05533 ↗
21. 10.1038/nmat231010.1038/nmat2310 ↗
22. 10.1021/ja042353u10.1021/ja042353u ↗
23. 10.1021/ja074841i10.1021/ja074841i ↗
24. 10.1002/adma.20080203110.1002/adma.200802031 ↗
25. 10.1073/pnas.060503310310.1073/pnas.0605033103 ↗
26. 10.1021/ja067879o10.1021/ja067879o ↗
27. 10.1038/nmat161210.1038/nmat1612 ↗
28. 10.1021/ja075242e10.1021/ja075242e ↗
29. 10.1002/adma.20090145410.1002/adma.200901454 ↗
30. 10.1038/3500660310.1038/35006603 ↗
31. 10.1038/nature0772710.1038/nature07727 ↗
32. 10.1021/ja809555c10.1021/ja809555c ↗
33. 10.1002/adma.20070006410.1002/adma.200700064 ↗
34. 10.1002/cphc.20030088210.1002/cphc.200300882 ↗
35. 10.1002/anie.20046132410.1002/anie.200461324 ↗
36. 10.1021/jp046246y10.1021/jp046246y ↗
37. 10.1063/1.171072910.1063/1.1710729 ↗
38. 10.1063/1.204325610.1063/1.2043256 ↗
39. 10.1021/ja901077a10.1021/ja901077a ↗
40. 10.1007/s00339-008-5024-y10.1007/s00339-008-5024-y ↗
41. 10.1021/ja809848y10.1021/ja809848y ↗
42. 10.1063/1.217762710.1063/1.2177627 ↗
43. 10.1109/LED.2006.88101910.1109/LED.2006.881019 ↗
44. 10.1038/nmat257010.1038/nmat2570 ↗
45. 10.1002/adma.20080062910.1002/adma.200800629 ↗
46. Parafocusing Bragg–Brentano grants high‐resolution and quite narrow peaks but high preferred‐orientation effects whereas Debye–Scherrer geometry mounting a glass capillary loaded with ground PD18‐CN2 crystals affords correct estimates of the measured intensities at the expense of evident peak broadening (by sample‐effect contribution).
47. 10.1107/S010827018609681610.1107/S0108270186096816 ↗
48. 10.1098/rspa.1942.006310.1098/rspa.1942.0063 ↗
49. Apparently as derived from the preferred orientation coefficients employed in matching the experimental versus the calculated data for the X‐ray trace collected in flat‐plate geometry the needles elongate approximately in the [100] direction a not‐so‐obvious and difficult‐to‐interpret direction. However a few tests performed with different preferred orientation poles within the March– Dollase formulation show that the alternative [−651]. choice is only partially detrimental to the overall fitting thus suggesting the possible coincidence of the stacking and needle growth directions.
50. March A. Z. · Kristallografiya · 1932 · 81 · 285
51. 10.1107/S002188988608945810.1107/S0021889886089458 ↗
52. 10.1351/pac19651103037110.1351/pac196511030371 ↗
53. 10.1002/adfm.20070104510.1002/adfm.200701045 ↗
54. 10.1021/nl071495u10.1021/nl071495u ↗
55. 10.1021/jp061102010.1021/jp0611020 ↗
56. 10.1021/jp801749n10.1021/jp801749n ↗
57. Warren B. E. · 1990
58. 10.1103/PhysRevB.70.12540110.1103/PhysRevB.70.125401 ↗
59. 10.1021/ja044078h10.1021/ja044078h ↗
60. 10.1107/S002188980800106410.1107/S0021889808001064 ↗
61. 10.1021/jp808037w10.1021/jp808037w ↗
62. 10.1021/la803018210.1021/la8030182 ↗
63. 10.1021/jp973206410.1021/jp9732064 ↗
64. 10.1021/ja000991g10.1021/ja000991g ↗
65. 10.1016/j.physa.2004.05.02710.1016/j.physa.2004.05.027 ↗
66. 10.1103/PhysRevLett.90.01610410.1103/PhysRevLett.90.016104 ↗
67. 10.1002/pssr.20080205210.1002/pssr.200802052 ↗
68. 10.1016/j.susc.2010.11.01810.1016/j.susc.2010.11.018 ↗
69. 10.1063/1.12623610.1063/1.126236 ↗
70. 10.1103/PhysRevLett.70.327110.1103/PhysRevLett.70.3271 ↗
71. 10.1103/PhysRevLett.66.234810.1103/PhysRevLett.66.2348 ↗
72. 10.1103/PhysRevE.51.188910.1103/PhysRevE.51.1889 ↗
73. 10.1103/PhysRevB.61.769210.1103/PhysRevB.61.7692 ↗
74. 10.1103/PhysRevLett.69.376210.1103/PhysRevLett.69.3762 ↗
75. 10.1103/PhysRevLett.78.238910.1103/PhysRevLett.78.2389 ↗
76. 10.1364/JOSAA.5.00009910.1364/JOSAA.5.000099 ↗
77. 10.1103/PhysRevB.52.1486810.1103/PhysRevB.52.14868 ↗
78. 10.1080/1058725960803190610.1080/10587259608031906 ↗
79. 10.1063/1.295190010.1063/1.2951900 ↗
80. 10.1103/PhysRevB.4.104110.1103/PhysRevB.4.1041 ↗
81. 10.1103/PhysRevB.25.83410.1103/PhysRevB.25.834 ↗
82. 10.1002/pssr.20070122110.1002/pssr.200701221 ↗
83. 10.1063/1.182622910.1063/1.1826229 ↗
84. 10.1039/b804317e10.1039/b804317e ↗
85. 10.1039/b810993a10.1039/b810993a ↗
86. 10.1002/adma.20100144610.1002/adma.201001446 ↗
87. 10.1016/j.nimb.2005.12.04210.1016/j.nimb.2005.12.042 ↗
88. 10.1016/j.nimb.2005.12.00810.1016/j.nimb.2005.12.008 ↗
89. 10.1201/978142000801210.1201/9781420008012 ↗
90. 10.1016/j.orgel.2011.01.01610.1016/j.orgel.2011.01.016 ↗
91. 10.1038/nature0337610.1038/nature03376 ↗
92. 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 ↗
93. Vissenberg M. C. J. M. · Phys. Rev. B: Condens. Matter · 1998 · 57 · 2964
94. 10.1063/1.150843610.1063/1.1508436 ↗
95. 10.1016/S0379-6779(02)00398-310.1016/S0379-6779(02)00398-3 ↗
96. 10.1016/0379-6779(94)90075-210.1016/0379-6779(94)90075-2 ↗
97. Gwyddion Scan Probe Microscopy data analysis software.
98. Frisch M . J. · 2004
99. 10.1080/089270203100010488710.1080/0892702031000104887 ↗
100. 10.1021/j100389a01010.1021/j100389a010 ↗