Controllable Supramolecular Architectures for Modulating Optical Properties on the Molecular Aggregation Level

2014 ◽  
Vol 2014 (23) ◽  
pp. 5004-5009 ◽  
Author(s):  
Runsheng Jiang ◽  
Zheng Xue ◽  
Yongjun Li ◽  
Zhihong Qin ◽  
Yuliang Li ◽  
...  
2018 ◽  
Vol 122 (7) ◽  
pp. 3965-3969 ◽  
Author(s):  
A. Saaidia ◽  
M. A. Saidani ◽  
E. Hleli ◽  
S. Alam ◽  
C. Ulbricht ◽  
...  

2015 ◽  
Vol 119 (43) ◽  
pp. 24643-24648 ◽  
Author(s):  
Fatima Bencheikh ◽  
David Duché ◽  
Carmen M. Ruiz ◽  
Jean-Jacques Simon ◽  
Ludovic Escoubas

2016 ◽  
Vol 4 (34) ◽  
pp. 8006-8013 ◽  
Author(s):  
Shian Ying ◽  
Mingshuai Chen ◽  
Zhongwei Liu ◽  
Kai Zhang ◽  
Yuyu Pan ◽  
...  

The conjugation bridges of DPP derivatives could significantly tune and alter molecular aggregation behaviors and fluorescence properties.


2021 ◽  
Vol 186 ◽  
pp. 109036
Author(s):  
K. Waszkowska ◽  
Y. Cheret ◽  
A. Zawadzka ◽  
A. Korcala ◽  
J. Strzelecki ◽  
...  

2008 ◽  
Vol 6 (4) ◽  
pp. 569-574 ◽  
Author(s):  
Juraj Bujdák ◽  
Nobuo Iyi

AbstractFormamide colloidal suspensions of layered double hydroxides (LDHs) with anionic dye, meso-tetrakis(4-sulfonatophenyl)porphine (TPPS) were prepared. Optical properties of these suspensions were investigated by means of absorption and fluorescence spectroscopies in the visible region. For more detailed characterization, second derivative curves of the spectra were calculated. The adsorption of the dye on LDH nanosheets led to partial molecular aggregation, reflected in significant changes of the dye optical properties. The Soret band in the absorption spectra was split into two peaks and decreased in intensity. Changes were observed also for the Q-bands. The molecular aggregation significantly quenched the emission of the dye. The low intensity emission from dye H-aggregates was identified at slightly longer wavelengths. The molecular aggregation increased with the dye/LDH ratio. At low dye loadings, the optical properties were very similar to the dye solution. The yields of the dye molecular aggregation increased with LDH surface charge.


2021 ◽  
pp. 109551
Author(s):  
Fabián Cuétara-Guadarrama ◽  
Mireille Vonlanthen ◽  
Kendra Sorroza-Martínez ◽  
Israel González-Méndez ◽  
Ernesto Rivera

2019 ◽  
Vol 21 (23) ◽  
pp. 12091-12099 ◽  
Author(s):  
Hussein Fakhouri ◽  
Martina Perić ◽  
Franck Bertorelle ◽  
Philippe Dugourd ◽  
Xavier Dagany ◽  
...  

The ability of gold(i) thiolates to self-assemble into supramolecular architectures opens the route for a new class of nanomaterials with a unique structure–optical property relationship.


2015 ◽  
Vol 3 (9) ◽  
pp. 2065-2071 ◽  
Author(s):  
F. D. Fleischli ◽  
N. Ghasdian ◽  
T. K. Georgiou ◽  
N. Stingelin

Here we demonstrate that the use of macrosurfactants in the production of poly(3-hexylthiophene) (P3HT):water dispersion allows to drastically change the semiconductor's molecular aggregation, leading to pronounced H- or J-like behaviour depending on the macrosurfactant used and the conditions selected to produce the dispersions.


Author(s):  
K. Tsuno ◽  
T. Honda ◽  
Y. Harada ◽  
M. Naruse

Developement of computer technology provides much improvements on electron microscopy, such as simulation of images, reconstruction of images and automatic controll of microscopes (auto-focussing and auto-correction of astigmatism) and design of electron microscope lenses by using a finite element method (FEM). In this investigation, procedures for simulating the optical properties of objective lenses of HREM and the characteristics of the new lens for HREM at 200 kV are described.The process for designing the objective lens is divided into three stages. Stage 1 is the process for estimating the optical properties of the lens. Firstly, calculation by FEM is made for simulating the axial magnetic field distributions Bzc of the lens. Secondly, electron ray trajectory is numerically calculated by using Bzc. And lastly, using Bzc and ray trajectory, spherical and chromatic aberration coefficients Cs and Cc are numerically calculated. Above calculations are repeated by changing the shape of lens until! to find an optimum aberration coefficients.


Author(s):  
A. Strojnik ◽  
J.W. Scholl ◽  
V. Bevc

The electron accelerator, as inserted between the electron source (injector) and the imaging column of the HVEM, is usually a strong lens and should be optimized in order to ensure high brightness over a wide range of accelerating voltages and illuminating conditions. This is especially true in the case of the STEM where the brightness directly determines the highest resolution attainable. In the past, the optical behavior of accelerators was usually determined for a particular configuration. During the development of the accelerator for the Arizona 1 MEV STEM, systematic investigation was made of the major optical properties for a variety of electrode configurations, number of stages N, accelerating voltages, 1 and 10 MEV, and a range of injection voltages ϕ0 = 1, 3, 10, 30, 100, 300 kV).


Sign in / Sign up

Export Citation Format

Share Document