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Optical properties versus

Figure Bl.26.14. Plot of A versus K, the imaginary part of the refractive index. (B) MEASUREMENT OF FILM THICKNESS AND OPTICAL PROPERTIES... Figure Bl.26.14. Plot of A versus K, the imaginary part of the refractive index. (B) MEASUREMENT OF FILM THICKNESS AND OPTICAL PROPERTIES...
Figure 11.2. Nanowire electronic and optical properties, (a) Schematic of an NW-FET used to characterize electrical transport properties of individual NWs. (inset) SEM image of an NW-FET two metal electrodes, which correspond to source and drain, are visible at the left and right sides of the image, (b) Current versus voltage for an n-type InP NW-FET. The numbers inside the plot indicate the corresponding gate voltages (Vg). The inset shows current versus Vg for Fsd of 0.1 V. (c) Real-color photoluminescence image of various NWs shows different color emissions, (d) Spectra of individual NW photoluminescence. All NW materials show a clean band-edge emission spectrum with narrow FWHM around 20nm. (See color insert.)... Figure 11.2. Nanowire electronic and optical properties, (a) Schematic of an NW-FET used to characterize electrical transport properties of individual NWs. (inset) SEM image of an NW-FET two metal electrodes, which correspond to source and drain, are visible at the left and right sides of the image, (b) Current versus voltage for an n-type InP NW-FET. The numbers inside the plot indicate the corresponding gate voltages (Vg). The inset shows current versus Vg for Fsd of 0.1 V. (c) Real-color photoluminescence image of various NWs shows different color emissions, (d) Spectra of individual NW photoluminescence. All NW materials show a clean band-edge emission spectrum with narrow FWHM around 20nm. (See color insert.)...
The mass versus particle size distribution of several polymer latices with diameters in the range of 30 nm to 1500 nm was determined in less than 20 minutes using an integrated hydrodynamic chromatograph. Distributions obtained were compared with those found by other particle sizing techniques such as electron microscopy to verify validity of the technique. The instrument employed was able to analyze latices re-producibly with different optical properties, even though some of the injected particles may have been trapped within the column. Latex properties were correlated with particle size distribution data to illustrate the benefit of this particle sizing technique. [Pg.256]

The foregoing remarks show that optical properties of organic conductors, in particular their UV-VIS, Raman, and IR spectra, can be used to estimate a number of physical parameters and among other things, the formal charge of the molecules or ions their evolution versus temperature, CT reactions, and so on, can be studied as well. Besides, examination of the IR spectra of low-dimensional organic conductors permits one to draw some conclusions about the stoichiometry and electronic properties of the salt. [Pg.243]

Comil, J. et ah, Charge transport versus optical properties in semiconducting crystalline... [Pg.218]

Apart from these intrinsic factors, due primarily to chiral nature of the skin components, extrinsic factors such as differences in physicochemical properties between enantiomers and racemate have been reported to cause stereoselective permeation, particularly with respect to individual optical isomers versus their racemates [38]. In addition to differences in the physicochemical properties, other extrinsic factors were also implicated in the enantioselective permeation across the skin including (1) the presence of chiral permeation enhancers [32,33,39], (2) the presence of stereoselective retardants in the donor vehicle [40], (3) differences in the hydrolysis rates of the prodrugs of the enantiomers in epidermis/dermis [23-25], and (4) carrier mediated transport [41]. [Pg.91]

In view of the specific phase structure of the polymer irradiated, it is of interest to analyze the optical properties (extinction) of Ag nanoparticles embedded in the amorphous carbon matrix (C matrix). For this system, the extinction cross-section spectra versus particle size dependence (Figure 8.6)... [Pg.254]

The two electrons transferred from TDAE to PEDOT-PSS are expected to undope the conjugated polymer chains. Since TDAE diffuses into PEDOT-PSS, long exposures to the electron donor induce changes in the optical properties of the polymer film. Optical absorption experiments on 200 nm thick PEDOT-PSS films coated onto a transparent polyethylene terephthalate (PET) substrate. The pol5mier film was exposed to the TDAE vapor in an inert nitrogen atmosphere and shows the difference in absorption spectrum between a film exposed to TDAE and the pristine PEDOT-PSS layer (Figs. 3.10 and 3.11). The modification of the optical properties and the sheet resistance of the pol5mier layer were recorded versus exposure time. The two absorption features at 550 nm and... [Pg.81]

Figure 3.32. Calculated reflectivity AR/Rp for bands at 1240 cm (1-3) and 1090 cm" (4, 5) in p-polarized IRRAS spectrum Figure 3.32. Calculated reflectivity AR/Rp for bands at 1240 cm (1-3) and 1090 cm" (4, 5) in p-polarized IRRAS spectrum <p- = 71°) of SiOz layer on Si surface versus thickness of SiOz layer in assumption of (1) sharp surfaces, (2,4) gradient in optical properties of SiOz layer, and (3, 5) gradient in both SiOz layer and substrate (depth of transition layer in substrate with exponential variation of ns is equal to 50 nm). Reprinted, by permission, from V. P. Tolstoy and S. N. Gruzinov, Opt. Spectrosc. 71, 77-80 (1991), p. 78, Fig. 2. Copyright 1991 Optical Society of America.
J. Cornil, J. P. Calbert, D. Beljonne, R. Silbey, J. L. Bredas, Charge transport versus optical properties in semiconducting crystalline organic thin films, Adv. Mater., 12, 978-983 (2000). [Pg.416]


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