Spectroscopic Interrogation of Layer-by-layer Assembled Films of Conjugated Polyelectrolytes

2005 ◽  
Vol 23 (7) ◽  
pp. 925-927
Author(s):  
Wu Hai-Ping ◽  
Xu Hui ◽  
Fan Chun-Hai
Langmuir ◽  
2009 ◽  
Vol 25 (10) ◽  
pp. 5969-5973 ◽  
Author(s):  
Bin Sun ◽  
Yang Zhang ◽  
Ke-Jun Gu ◽  
Qun-Dong Shen ◽  
Yan Yang ◽  
...  

2021 ◽  
Author(s):  
◽  
Martin Edward Henry Heeley

<p>Conjugated Polyelectrolytes (CPEs) are a branch of conducting polymers that combine the electronic and solution processability of conjugated polymers (CPs) with the ionic and self-assembling nature of polyelectrolytes. These systems have been shown to exhibit high sensitivity with changes in aggregation state and optical character dependant on the local environment. The ionic character of the CPEs can be used as scaffolds for post-synthetic alterations allowing for control of the optical and physical characteristics. In this thesis, the control of the optical and physical characteristics of the conjugated polyelectrolytes (CPEs) sodium poly[2-(3-thienyl)ethoxyl-4-butylsulfonate] (PTEBS) and poly(9,9-bis[6-(N,N,N-trimethylammonium)hexyl]fluorine-co-altphenylene] (FPQ-X, where X denotes the various counter-ions of the polymers) is investigated though the addition of various extrinsic ions to dilute solutions and concentrated solutions used for film casting, with the main focus being in the solution phase behavior. The CPE characteristics were studied primarily through UV/Vis absorption and fluorescence spectroscopy coupled with dynamic light scattering and surface tension techniques. Controlling the solution phase characteristics of the CPE was investigated through a study of through of solvent composition effects, monovalent and divalent ion addition, organic salt addition, and surfactant additions to dilute aqueous solutions of the CPEs. Solvent composition effects were shown to result in fluorescence enhancement with changes in the polarity of the solvent, while the addition of monovalent and divalent ions was shown to induce fluorescence quenching through ionic strength, ion condensation, and cross-linking of CPE molecules dependant on the concentration and valency of the metal ion. Organic salt additions of a range of concentrations were shown to result in both concentration and alkyl chain length dependant fluorescence intensity enhancements with little changes in the particle size of aggregates in solution. The lack of change in particle size suggested that the effects were localized to the aggregate surface with the size of the organic salt inducing a steric prying effect on the CPE aggregate. A proposed model of this was created to this effect. Large changes in the optical and physical characteristics of the CPEs were found with addition of surfactants to the CPE solutions. Fluorescence quenching and enhancements, particle size increases and decreases, and absorption hypsochromic shifts have been noted, with surfactant structure and concentration dependence. The resulting effects are shown to be hydrophobically, electrostatically, and self-assembly driven. Concentration control of the CPE aggregate size and optical characteristics is completed with surfactant micelles being noted at pre-CMC concentrations within the solutions. A model of interactions at the various concentration levels of surfactant has been developed explaining these results. Transferring this system to the solid state has been shown to exhibit both bathochromic and hypsochromic shifts in absorption and have two optically active phases. The dual phase absorption and emission was attributed to a CPE-surfactant complex where the CPE backbone and surfactant self assemblies result in lamellar type structures within the cast films. The optical overlap of the emission and absorption of the CPEs used was also shown to be favorable for FRET based transfer from FPQ-X to PTEBS. Films created by the layer-by-layer technique showed FRET based signal of PTEBS via excitation of FPQ-Br showing effective FRET based energy transfer between the two species. The absorption signatures of the films with multiple layer-by-layer processes showed that the films do not result in unique layers but rather interdigitated mixtures within the film. Proof of concept P3HT with DOD addition OFET devices were then created in the attempt to alter the electrode potentials using mobile ions. The devices were found to be less efficient than that of the controls due to the disruption of self assembled structures within the devices hampering electron movement.</p>


Langmuir ◽  
2011 ◽  
Vol 27 (8) ◽  
pp. 5021-5028 ◽  
Author(s):  
Quentin Bricaud ◽  
Roxane M. Fabre ◽  
Robert N. Brookins ◽  
Kirk S. Schanze ◽  
John R. Reynolds

2021 ◽  
Author(s):  
◽  
Martin Edward Henry Heeley

<p>Conjugated Polyelectrolytes (CPEs) are a branch of conducting polymers that combine the electronic and solution processability of conjugated polymers (CPs) with the ionic and self-assembling nature of polyelectrolytes. These systems have been shown to exhibit high sensitivity with changes in aggregation state and optical character dependant on the local environment. The ionic character of the CPEs can be used as scaffolds for post-synthetic alterations allowing for control of the optical and physical characteristics. In this thesis, the control of the optical and physical characteristics of the conjugated polyelectrolytes (CPEs) sodium poly[2-(3-thienyl)ethoxyl-4-butylsulfonate] (PTEBS) and poly(9,9-bis[6-(N,N,N-trimethylammonium)hexyl]fluorine-co-altphenylene] (FPQ-X, where X denotes the various counter-ions of the polymers) is investigated though the addition of various extrinsic ions to dilute solutions and concentrated solutions used for film casting, with the main focus being in the solution phase behavior. The CPE characteristics were studied primarily through UV/Vis absorption and fluorescence spectroscopy coupled with dynamic light scattering and surface tension techniques. Controlling the solution phase characteristics of the CPE was investigated through a study of through of solvent composition effects, monovalent and divalent ion addition, organic salt addition, and surfactant additions to dilute aqueous solutions of the CPEs. Solvent composition effects were shown to result in fluorescence enhancement with changes in the polarity of the solvent, while the addition of monovalent and divalent ions was shown to induce fluorescence quenching through ionic strength, ion condensation, and cross-linking of CPE molecules dependant on the concentration and valency of the metal ion. Organic salt additions of a range of concentrations were shown to result in both concentration and alkyl chain length dependant fluorescence intensity enhancements with little changes in the particle size of aggregates in solution. The lack of change in particle size suggested that the effects were localized to the aggregate surface with the size of the organic salt inducing a steric prying effect on the CPE aggregate. A proposed model of this was created to this effect. Large changes in the optical and physical characteristics of the CPEs were found with addition of surfactants to the CPE solutions. Fluorescence quenching and enhancements, particle size increases and decreases, and absorption hypsochromic shifts have been noted, with surfactant structure and concentration dependence. The resulting effects are shown to be hydrophobically, electrostatically, and self-assembly driven. Concentration control of the CPE aggregate size and optical characteristics is completed with surfactant micelles being noted at pre-CMC concentrations within the solutions. A model of interactions at the various concentration levels of surfactant has been developed explaining these results. Transferring this system to the solid state has been shown to exhibit both bathochromic and hypsochromic shifts in absorption and have two optically active phases. The dual phase absorption and emission was attributed to a CPE-surfactant complex where the CPE backbone and surfactant self assemblies result in lamellar type structures within the cast films. The optical overlap of the emission and absorption of the CPEs used was also shown to be favorable for FRET based transfer from FPQ-X to PTEBS. Films created by the layer-by-layer technique showed FRET based signal of PTEBS via excitation of FPQ-Br showing effective FRET based energy transfer between the two species. The absorption signatures of the films with multiple layer-by-layer processes showed that the films do not result in unique layers but rather interdigitated mixtures within the film. Proof of concept P3HT with DOD addition OFET devices were then created in the attempt to alter the electrode potentials using mobile ions. The devices were found to be less efficient than that of the controls due to the disruption of self assembled structures within the devices hampering electron movement.</p>


Author(s):  
M.A. Parker ◽  
K.E. Johnson ◽  
C. Hwang ◽  
A. Bermea

We have reported the dependence of the magnetic and recording properties of CoPtCr recording media on the thickness of the Cr underlayer. It was inferred from XRD data that grain-to-grain epitaxy of the Cr with the CoPtCr was responsible for the interaction observed between these layers. However, no cross-sectional TEM (XTEM) work was performed to confirm this inference. In this paper, we report the application of new techniques for preparing XTEM specimens from actual magnetic recording disks, and for layer-by-layer micro-diffraction with an electron probe elongated parallel to the surface of the deposited structure which elucidate the effect of the crystallographic structure of the Cr on that of the CoPtCr.XTEM specimens were prepared from magnetic recording disks by modifying a technique used to prepare semiconductor specimens. After 3mm disks were prepared per the standard XTEM procedure, these disks were then lapped using a tripod polishing device. A grid with a single 1mmx2mm hole was then glued with M-bond 610 to the polished side of the disk.


Author(s):  
Yoshichika Bando ◽  
Takahito Terashima ◽  
Kenji Iijima ◽  
Kazunuki Yamamoto ◽  
Kazuto Hirata ◽  
...  

The high quality thin films of high-Tc superconducting oxide are necessary for elucidating the superconducting mechanism and for device application. The recent trend in the preparation of high-Tc films has been toward “in-situ” growth of the superconducting phase at relatively low temperatures. The purpose of “in-situ” growth is to attain surface smoothness suitable for fabricating film devices but also to obtain high quality film. We present the investigation on the initial growth manner of YBCO by in-situ reflective high energy electron diffraction (RHEED) technique and on the structural and superconducting properties of the resulting ultrathin films below 100Å. The epitaxial films have been grown on (100) plane of MgO and SrTiO, heated below 650°C by activated reactive evaporation. The in-situ RHEED observation and the intensity measurement was carried out during deposition of YBCO on the substrate at 650°C. The deposition rate was 0.8Å/s. Fig. 1 shows the RHEED patterns at every stage of deposition of YBCO on MgO(100). All the patterns exhibit the sharp streaks, indicating that the film surface is atomically smooth and the growth manner is layer-by-layer.


Author(s):  
S. Likharev ◽  
A. Kramarenko ◽  
V. Vybornov

At present time the interest is growing considerably for theoretical and experimental analysis of back-scattered electrons (BSE) energy spectra. It was discovered that a special angle and energy nitration of BSE flow could be used for increasing a spatial resolution of BSE mode, sample topography investigations and for layer-by layer visualizing of a depth structure. In the last case it was shown theoretically that in order to obtain suitable depth resolution it is necessary to select a part of BSE flow with the directions of velocities close to inverse to the primary beam and energies within a small window in the high-energy part of the whole spectrum.A wide range of such devices has been developed earlier, but all of them have considerable demerit: they can hardly be used with a standard SEM due to the necessity of sufficient SEM modifications like installation of large accessories in or out SEM chamber, mounting of specialized detector systems, input wires for high voltage supply, screening a primary beam from additional electromagnetic field, etc. In this report we present a new scheme of a compact BSE energy analyzer that is free of imperfections mentioned above.


Author(s):  
L. Hultman ◽  
C.-H. Choi ◽  
R. Kaspi ◽  
R. Ai ◽  
S.A. Barnett

III-V semiconductor films nucleate by the Stranski-Krastanov (SK) mechanism on Si substrates. Many of the extended defects present in the films are believed to result from the island formation and coalescence stage of SK growth. We have recently shown that low (-30 eV) energy, high flux (4 ions per deposited atom), Ar ion irradiation during nucleation of III-V semiconductors on Si substrates prolongs the 1ayer-by-layer stage of SK nucleation, leading to a decrease in extended defect densities. Furthermore, the epitaxial temperature was reduced by >100°C due to ion irradiation. The effect of ion bombardment on the nucleation mechanism was explained as being due to ion-induced dissociation of three-dimensional islands and ion-enhanced surface diffusion.For the case of InAs grown at 380°C on Si(100) (11% lattice mismatch), where island formation is expected after ≤ 1 monolayer (ML) during molecular beam epitaxy (MBE), in-situ reflection high-energy electron diffraction (RHEED) showed that 28 eV Ar ion irradiation prolonged the layer-by-layer stage of SK nucleation up to 10 ML. Otherion energies maintained layer-by-layer growth to lesser thicknesses. The ion-induced change in nucleation mechanism resulted in smoother surfaces and improved the crystalline perfection of thicker films as shown by transmission electron microscopy and X-ray rocking curve studies.


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