3 research outputs found
Morphological and Structural Investigation of Sexithiophene Growth on KCl (100)
The morphology and structure of sexithiophene deposited
on KCl
(100) substrates was investigated by scanning force microscopy and
specular X-ray diffraction measurements. Two different needle-like
structures with {010} and {4Ì…11} contact planes have been observed
as well as islands of almost upright standing sexithiophene molecules
with a {100} contact plane. Furthermore an azimuthal alignment of
all three crystal orientations was observed by X-ray diffraction pole
figure measurements, and the growth directions reflect the 4-fold
rotational symmetry of the substrate surface. In addition the analysis
of crystals with {4Ì…11} and {100} contact planes unveiled that
they share a common crystallographic direction which is explained
by ledge directed epitaxy
Epitaxy of Rodlike Organic Molecules on Sheet Silicatesî—¸A Growth Model Based on Experiments and Simulations
During the last years, self-assembled organic nanostructures have been recognized as a proper fundament for several electrical and optical applications. In particular, phenylenes deposited on muscovite mica have turned out to be an outstanding material combination. They tend to align parallel to each other forming needlelike structures. In that way, they provide the key for macroscopic highly polarized emission, waveguiding, and lasing. The resulting anisotropy has been interpreted so far by an induced dipole originating from the muscovite mica substrate. Based on a combined experimental and theoretical approach, we present an alternative growth model being able to explain molecular adsorption on sheet silicates in terms of molecule−surface interactions only. By a comprehensive comparison between experiments and simulations, we demonstrate that geometrical changes in the substrate surface or molecule lead to different molecular adsorption geometries and needle directions which can be predicted by our growth model
Color Tuning of Nanofibers by Periodic Organic–Organic Hetero-Epitaxy
We report on the epitaxial growth of periodic para-hexaphenyl (<i>p</i>-6P)/α-sexi-thiophene (6T) multilayer heterostructures on top of <i>p</i>-6P nanotemplates. By the chosen approach, 6T molecules are forced to align parallel to the <i>p</i>-6P template molecules, which yields highly polarized photoluminescence (PL)-emission of both species. The PL spectra show that the fabricated multilayer structures provide optical emission from two different 6T phases, interfacial 6T molecules, and 3-dimensional crystallites. By a periodical deposition of 6T monolayers and <i>p</i>-6P spacers it is demonstrated that the strongly polarized spectral contribution of interfacial 6T can be precisely controlled and amplified. By analyzing the PL emission of both 6T phases as a function of <i>p</i>-6P spacer thickness (Δ<i>d</i><sub><i>p</i>–6P</sub>) we have determined a critical value of Δ<i>d</i><sub><i>p</i>–6P </sub>≈ 2.73 nm where interfacial 6T runs into saturation and the surplus of 6T starts to cluster in 3-dimensional crystallites. These results are further substantiated by UPS and XRD measurements. Moreover, it is demonstrated by morphological investigations, provided by scanning force microscopy and fluorescence microscopy, that periodical deposition of 6T and <i>p</i>-6P leads to a significant improvement of homogeneity in PL-emission and morphology of nanofibers. Photoluminescence excitation experiments in combination with time-resolved photoluminescence demonstrate that the spectral emission of the organic multilayer nanofibers is dominated by a resonant energy transfer from <i>p</i>-6P host- to 6T guest-molecules. The sensitization time of the 6T emission in the 6T/<i>p</i>-6P multilayer structures depends on the <i>p</i>-6P spacer thickness, and can be explained by well separated layers of host–guest molecules obtained by organic–organic heteroepitaxy. The spectral emission and consequently the fluorescent color of the nanofibers can be efficiently tuned from the blue <i>via</i> white to the yellow-green spectral range