2013
DOI: 10.1002/ange.201302894
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Controlling the Structures and Photonic Properties of Organic Nanomaterials by Molecular Design

Abstract: Stapelkunde: Zwei verschiedene, aber verwandte Naphthalene bilden, gesteuert durch ihre H‐Brückenbindungen und π‐π‐Stapelung, unterschiedliche Nanostrukturen (siehe Bild). Diese Nanostrukturen wiesen einzigartige Merkmale hinsichtlich photonischer Begrenzung und Lichtweiterleitung auf, was einen Einsatz in nanophotonischen Schaltkreisen nahelegt.

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Cited by 58 publications
(13 citation statements)
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“…Recently Zhao et al. observed the asymmetric light propagation in rhombic organic microplates of 2‐acetyl‐6‐methylaminonaphthalene (AMN), due to the anisotropic molecular packing 20. Spano calculated that the transition dipole moment of DSB molecule is almost parallel to the long molecular axis (Figure S5b) 14.…”
mentioning
confidence: 99%
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“…Recently Zhao et al. observed the asymmetric light propagation in rhombic organic microplates of 2‐acetyl‐6‐methylaminonaphthalene (AMN), due to the anisotropic molecular packing 20. Spano calculated that the transition dipole moment of DSB molecule is almost parallel to the long molecular axis (Figure S5b) 14.…”
mentioning
confidence: 99%
“…According to the TIR theory, the larger n r =2.1 at the HMD/air interface than n r =1.45 at the HMD/quartz interface results in a higher TIR efficiency and a weaker optical loss at the HMD top‐face than those at the HMD bottom‐face 21. Therefore, asymmetric light propagation takes place 20. After the obliquely upward guided PL undergoes TIR at the top‐face, it could be further reflected by the given side‐face (Face 1), and be coupled into 3‐WGM or D3‐WGM resonators selectively constituted by three facets (Face 1, Face 3, and Face 5) (see Figure S5c); however, the obliquely downward guided PL would tend to be leaked into quartz substrate 21.…”
mentioning
confidence: 99%
“…As the distance (D) between the excitation point (I body ) and the data collection point (I tip ) increased, the fluorescence intensity decreased gradually, accompanied by a slight red-shift (self-absorption caused by the overlap between absorption and emission wavelength) (Figure 4 a-b, Figure S11). [53,54] The optical loss coefficient of DBDT crystal was calculated through the equation I tip /I body = exp(αD). α (mm À 1 ) was the optical loss coefficient.…”
Section: Resultsmentioning
confidence: 99%
“…Preparation of p‐DTS(FBTTh 2 ) 2 Microwires : A simple solution‐phase self‐assembly procedure was used that involves application of different solvents and a slow decrease in temperature . Specifically, 100 µL of p ‐DTS(FBTTh 2 ) 2 chlorobenzene solution (2 mg mL −1 , good solvent) was rapidly injected into 2 mL of hexane as the poor solvent at 60 °C.…”
Section: Methodsmentioning
confidence: 99%