Abstract:International audienceThe optical response of rubrene crystals is described by providing the full UV-VIS dielectric tensor. Consistently with the molecular and crystal symmetries, the lowest crystal transition originates from an Au molecular transition, it is polarized along the c axis (normal to the larger crystal face), and it is the origin of the emission, which is self-guided towards the edge where the corresponding polarization and intensity angular distribution are detected. By contrast, the Bu molecular… Show more
“…The directions of polarization of the M-and L-axes can be considered as c-and b-axes, respectively, in a rubrene single crystal. [30][31][32] In the LCM PL spectra obtained from the edge of both single crystals (i.e., area (1) in Fig. 4a and b), the LCM PL peak at 572 nm was stronger than that at 601 nm, as shown in Figure 4c and d. However, the LCM PL peaks from the inside (i.e., areas (2) and (3) in Fig.…”
Section: Lcm Pl Characteristics On the Nanometer Scalementioning
confidence: 78%
“…We also observed the relatively long free-charge-carrier tail at a longer wavelength (!580 nm) for the rubrene nanowires. [30][31][32] The UV/ Vis absorption peaks of higher-order vibronic bands were regularly spaced, with E Ã 0-n ¼ E Ã 0-0 þ n£v C-C (i.e., 2.38, 2.55, and 2.72 eV), where n is an integer, by an energy corresponding to the C-C stretch vibration modes (£v C-C ¼ 0.17 eV). [32] The UV/ Vis absorption peaks for rubrene nanowires were similar with those of the rubrene single crystal reported earlier.…”
Section: Structural Optical and Electricalmentioning
This is a report on a new method of growth of a light‐emitting rubrene nanowires array with diameters of 200 ± 10 nm by using organic vapor transport through Al2O3 nanoporous templates. Nanometer‐scale laser confocal microscope (LCM) photoluminescence (PL) spectra and crystalline structures of the rubrene nanowires are compared with those of rubrene single crystals prepared with the same experimental conditions without the template. In the LCM PL spectra it is observed that the PL spectra and intensity varies with the detecting positions because of the crystal growth characteristics of the rubrene molecules. A single rubrene nanowire has a wider LCM PL band width than that of the rubrene single crystal. This may originate from the light emissions of the mixed polarized bands due to additional new crystallinity in the formation of the nanowires. From the current–voltage characteristic curves, the semiconducting nature of both the rubrene nanowires and single crystals is observed.
“…The directions of polarization of the M-and L-axes can be considered as c-and b-axes, respectively, in a rubrene single crystal. [30][31][32] In the LCM PL spectra obtained from the edge of both single crystals (i.e., area (1) in Fig. 4a and b), the LCM PL peak at 572 nm was stronger than that at 601 nm, as shown in Figure 4c and d. However, the LCM PL peaks from the inside (i.e., areas (2) and (3) in Fig.…”
Section: Lcm Pl Characteristics On the Nanometer Scalementioning
confidence: 78%
“…We also observed the relatively long free-charge-carrier tail at a longer wavelength (!580 nm) for the rubrene nanowires. [30][31][32] The UV/ Vis absorption peaks of higher-order vibronic bands were regularly spaced, with E Ã 0-n ¼ E Ã 0-0 þ n£v C-C (i.e., 2.38, 2.55, and 2.72 eV), where n is an integer, by an energy corresponding to the C-C stretch vibration modes (£v C-C ¼ 0.17 eV). [32] The UV/ Vis absorption peaks for rubrene nanowires were similar with those of the rubrene single crystal reported earlier.…”
Section: Structural Optical and Electricalmentioning
This is a report on a new method of growth of a light‐emitting rubrene nanowires array with diameters of 200 ± 10 nm by using organic vapor transport through Al2O3 nanoporous templates. Nanometer‐scale laser confocal microscope (LCM) photoluminescence (PL) spectra and crystalline structures of the rubrene nanowires are compared with those of rubrene single crystals prepared with the same experimental conditions without the template. In the LCM PL spectra it is observed that the PL spectra and intensity varies with the detecting positions because of the crystal growth characteristics of the rubrene molecules. A single rubrene nanowire has a wider LCM PL band width than that of the rubrene single crystal. This may originate from the light emissions of the mixed polarized bands due to additional new crystallinity in the formation of the nanowires. From the current–voltage characteristic curves, the semiconducting nature of both the rubrene nanowires and single crystals is observed.
“…[26][27][28] while those for the organic semiconductors rubrene, pentacene, and poly(3-hyxylthiophene) (P3HT) are 3.3-3.9, 2.6, and 4.4, respectively. [29][30][31] The derived value of ~5 lies between the two groups and possibly reflects the weaker ionic or stronger covalent character of CuSCN due to the -SCN constituent.…”
Section: Metal-insulator-semiconductor Capacitors Based On Cuscnmentioning
Wide band gap hole-transporting semiconductor copper(I) thiocyanate (CuSCN) has recently shown promise both as a transparent p-type channel material for thin-film transistors
“…Tavazzi et al [9,10] deduced anisotropic refractive index dispersions of rubrene along its crystal axes by fitting ellipsometry data. Their data ranged ~2.1−4.4 eV (~282−590 nm).…”
We have determined refractive indices of rubrene crystals in the wavelength regions where their emissions were observed. For this purpose, we grew in a vapor phase the rubrene crystals having both horizontal and vertical pairs of parallel crystal facets. The facets functioned as optical resonators that produced interference fringes in the emission and reflectance spectra. From the fringes in the emission spectrum, we estimated the dispersion of the phase refractive index along the crystal a-axis. The anisotropic group refractive indices were evaluated along the b-and c-axes from the fringes in the reflectance spectra. The experimental indices were compared with those computed from the density functional theory.
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