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Photoluminescence spectroscopy system

Finally, we will concentrate on the chemical reactivity of silyl derivatives of thiophene. The oxidative polymerization of various silyl monomers lead to polythiophene. The evaluation of this new polymerization reaction implies a precise characterization of the produced conjugated materials. Knowledge and the control of the pertinent parameters which direct the properties of the conjugated systems are essential. Also required is the development of methods which allow a precise characterization of the samples. The role of vibrational infrared and Raman spectroscopy is of fundamental importance in this field. Optical spectroscopy is one of the few tools for unravelling the structure of these materials and understanding their properties. First, new criteria based on infrared, Raman and photoluminescence spectroscopy which allow precise estimates of the conjugation properties will be reported. Then the synthesis and characterization of polythiophene samples arising from the oxidative polymerization of silyl thiophene will be presented. [Pg.627]

Andohna CM, Holthoff WG, Page PM, Mathews RA, Morrow JR, Bright FV. Spectroscopic system for direct lanthanide photoluminescence spectroscopy with nanomolar detection limits. Appl Spectrosc. 2009 63(5) 483 93. [Pg.327]

Photoelectron spectra of Cd compounds have been reported see Photoelectron Spectroscopy of Transition Metal Systems), but discrepancies have been noted. X-ray photoelectron spectroscopy has been used in surface studies. Simmetry, bond length, and eqnUibrium constants see Equilibrium Constant) of Cd complexes have been determined through IR and Raman spectroscopy. Resonance Raman spectroscopy and Photoluminescence allow investigation of the optical properties of ultrathin CdS films. Electron diffraction studies have been reported. ... [Pg.528]

Fluorescence and phosphorescence are emission processes which originate directly or indirectly (see 5 section ll.B) from the electronically excited singlet state and triplet state, respectively, produced by charge-transfer processes (Eqs. 1 and 2). Many publications deal with such charge-transfer transitions by diffuse reflectance spectroscopy (DRS) (2-6) showing the link between the latter technique and photoluminescence. It is worthwhile to recall that the emergence of the coordination chemistry of solid-state anions, namely, of surface lattice oxide ions, has almost entirely been based on the results of both photoluminescence and DRS analyses (7, 66). For some catalytic systems, vibrational structures can be detected (see Section IV.B) with an associated vibrational constant, which may be determined directly and independently by IR or Raman spectroscopy, evidencing the relation between these spectroscopies and photoluminescence (33, 34). [Pg.245]

When investigating the PFB F8BT system above we also used photoluminescence excitation spectroscopy to directly show the energy transfer to the exciplex. This is not possible here because of the very similar emission spectra of the F8BT exciton and the long-lived exciplex emission. The reasons for this similarity will be discussed in Section 2.2. We therefore conclude that the heterojunction between TFB and F8BT also supports exciplex formation. [Pg.51]

In Section 2.1.4, the electronic and photophysical properties of donor-acceptor or type-II heterojunctions between two semiconductor polymers were investigated. Exciplex formation was found to be a general phenomenon for type-II heterojunctions between polyfluorene copolymers. These are among the most widely used materials in polymer optoelectronics, but the presence of exciplexes had not yet been fully appreciated. This is because the exciplex population is often depopulated via efficient endothermic transfer towards the exciton, which leads to bulk exciton instead of exciplex emission. However, via time- and temperature-depen-dent photoluminescence (PL) spectroscopy the exciplex states can be identified. Employing a relationship known from small-molecule solution systems that relates the relative HOMO and LUMO levels of the molecules to the exciplex emis-... [Pg.86]

The nanocrystalline semiconductors, PbS and CuS, were prepared by y-irradiation at room temperature in an ethanol system by Qiao et al. (1999). Carbon disulfide was used as the sulfur source lead acetate and copper chloride were used as metal ion sources. The purity and compositions of the products were examined by x-ray photoelectron spectroscopy. The photoluminescence property of as-prepared PbS was further studied. A blue shift observed in the PL spectra indicated the quantum size effect on nanocrystalline PbS. [Pg.521]

Luminescence Spectroscopy. Photoluminescence measurements were performed with the aid of a Fluorolog3 spectro-fluorometer Fl3—22 (Horibajobin Yvon) equipped with double Czerny—Turner monochromators, a 450 W xenon lamp and a R928P photomultiplier with a photon counting system. Cooling down to 10 K was achieved by a closed cycle He cryostat (Janis Research). All emission spectra were corrected for the photomultiplier sensitivity and all excitation spectra for the intensity of the excitation source. To avoid any contamination of water on the sample s surfaces, we carried out the measurements in silica ampules with extreme purity which show no luminescence of the ampules itself. Reflection spectra were recorded on a Cary 5000 UV—vis—NIR spectrophotometer (Varian), which were corrected for both the lamp intensity and the photomultiplier sensitivity. [Pg.3]


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See also in sourсe #XX -- [ Pg.19 , Pg.20 ]




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