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Band position

Make measurements of band positions in the ultraviolet photoelectron spectmm in Figure 8.7 as accurately as you can and use these to determine cOg and cOgXg (Equations 7.82 and 6.18) for the ground electronic state of Hj. [Pg.334]

The shape of the broad absorption curve in Figure 9.17 is typical of that of any dye suitable for a laser. It shows an absorption maximum to low wavelength of the Og band position, which is close to the absorption-fluorescence crossing point. The shape of the absorption curve results from a change of shape of the molecule, from Sq to 5i, in the... [Pg.360]

Q are the absorbance and wavenumber, respectively, at the peak (center) of the band, p is the wavenumber, and y is the half width of the band at half height. Liquid band positions ate usually shifted slightly downward from vapor positions. Both band positions and widths of solute spectra are affected by solute—solvent interactions. Spectra of soHd-phase samples are similar to those of Hquids, but intermolecular interactions in soHds can be nonisotropic. In spectra of crystalline samples, vibrational bands tend to be sharper and may spHt in two, and new bands may also appear. If polarized infrared radiation is used, both crystalline samples and stressed amorphous samples (such as a stretched polymer film) show directional effects (28,29). [Pg.197]

Raman spectroscopy of graphite can be an experimental challenge, because the material is a strong blackbody absorber. Generally, low (1—10-mW) laser power is used to minimise heating, which causes the band positions to change. In addition, the expansion of the graphite causes the material to go out of the focus of the optical system, an effect which can be more pronounced in microprobe work. [Pg.213]

If the perturbations thus caused are relatively slight, the accepted perturbation theory can be used to interpret observed spectral changes (3,10,39). The spectral effect is calculated as the difference of the long-wavelength band positions for the perturbed and the initial dyes. In a general form, the band maximum shift, AX, can be derived from equation 4 analogous to the weU-known Hammett equation. Here p is a characteristic of an unperturbed molecule, eg, the electron density or bond order change on excitation or the difference between the frontier level and the level of the substitution. The other parameter. O, is an estimate of the perturbation. [Pg.494]

Also, using dyes as laser media or passive mode-locked compounds requires numerous special parameters, the most important of which ate the band position and bandwidth of absorption and fluorescence, the luminiscence quantum efficiency, the Stokes shift, the possibiHty of photoisomerization, chemical stabiHty, and photostabiHty. AppHcations of PMDs in other technical or scientific areas have additional special requirements. [Pg.499]

In Raman spectroscopy the intensity of scattered radiation depends not only on the polarizability and concentration of the analyte molecules, but also on the optical properties of the sample and the adjustment of the instrument. Absolute Raman intensities are not, therefore, inherently a very accurate measure of concentration. These intensities are, of course, useful for quantification under well-defined experimental conditions and for well characterized samples otherwise relative intensities should be used instead. Raman bands of the major component, the solvent, or another component of known concentration can be used as internal standards. For isotropic phases, intensity ratios of Raman bands of the analyte and the reference compound depend linearly on the concentration ratio over a wide concentration range and are, therefore, very well-suited for quantification. Changes of temperature and the refractive index of the sample can, however, influence Raman intensities, and the band positions can be shifted by different solvation at higher concentrations or... [Pg.259]

Figure 6.33 gives an overview of the changes in d band position for monolayers of one metal on top of another, as calculated by N0rskov and co-workers [A.V. Ruban, B. Hammer, P. Stoltze, K.W. Jacobsen, H.L. Shriver and J.K. N0rskov, J. Mol. Catal. A115 (1997)... [Pg.253]

Fig. 5.20 Schematic diagram illustrating the energy levels of different-sized CdSe quantum dots and Ti02 (band positions are not drawn to scale). The injection of electrons from CdSe into Ti02 is influenced by the energy difference between the two conduction bands. [Adapted (in gray scale) from [351]]... Fig. 5.20 Schematic diagram illustrating the energy levels of different-sized CdSe quantum dots and Ti02 (band positions are not drawn to scale). The injection of electrons from CdSe into Ti02 is influenced by the energy difference between the two conduction bands. [Adapted (in gray scale) from [351]]...
Raman Band Positions (cm ) IR Band Positions (cm ) Assignments... [Pg.33]

Figure 3.17 presents ps-TR spectra of the olehnic C=C Raman band region (a) and the low wavenumber anti-Stokes and Stokes region (b) of Si-rra i-stilbene in chloroform solution obtained at selected time delays upto 100 ps. Inspection of Figure 3.17 (a) shows that the Raman bandwidths narrow and the band positions up-shift for the olehnic C=C stretch Raman band over the hrst 20-30 ps. Similarly, the ratios of the Raman intensity in the anti-Stokes and Stokes Raman bands in the low frequency region also vary noticeably in the hrst 20-30 ps. In order to better understand the time-dependent changes in the Raman band positions and anti-Stokes/Stokes intensity ratios, a least squares htting of Lorentzian band shapes to the spectral bands of interest was performed to determine the Raman band positions for the olehnic... [Pg.149]

Figure 3.35. Time-resolved UVRR difference spectra (pump+prohe minus probe only) at the indicated times (ps) following the photolysis of HbCO. For display purposes, the top four traces were multiplied by a scale factor of 0.5. Band positions and assignments are marked at the top. (Reprinted from reference [156]. Copyright (2004), with permission from Elsevier.)... Figure 3.35. Time-resolved UVRR difference spectra (pump+prohe minus probe only) at the indicated times (ps) following the photolysis of HbCO. For display purposes, the top four traces were multiplied by a scale factor of 0.5. Band positions and assignments are marked at the top. (Reprinted from reference [156]. Copyright (2004), with permission from Elsevier.)...
As demonstrated in the two previous sections, TRIR spectroscopy can be used to provide direct structural information concerning organic reactive intermediates in solution as well as kinetic insight into mechanisms of prodnct formation. TRIR spectroscopy can also be used to examine solvent effects by revealing the inflnence of solvent on IR band positions and intensities. For example, TRIR spectroscopy has been used to examine the solvent dependence of some carbonylcarbene singlet-triplet energy gaps. Here, we will focns on TRIR stndies of specific solvation of carbenes. [Pg.198]

Table 4.2. Band position (cm ) of species arising from C02 adsorption at room temperature [69]... Table 4.2. Band position (cm ) of species arising from C02 adsorption at room temperature [69]...
Fig. 25. XPS valence band spectra for reactively sputtered Ru Ir, x02 electrodes on a Ti substrate after preparation for different compositions x. Note the shift in t2g band position. After [83]. Fig. 25. XPS valence band spectra for reactively sputtered Ru Ir, x02 electrodes on a Ti substrate after preparation for different compositions x. Note the shift in t2g band position. After [83].
The narrowest PFI bands in the present study are 3 cm-1 FWHM, using a 0.5 V/cm extraction field with the lasers attenuated to minimize effects of space charge. We measure band positions at the intensity maxima. These are reproducible to better than 1 cm-1. The bandwidth is limited by the rotational contour and also by the ionization process. A major advantage of ZEKE-PFI over more traditional photoelectron techniques is that the energy calibration is that of the tunable dye lasers, which are quite stable from day to day. In contrast, both electrostatic analyzers and time-of-flight photoelectron spectrometers require frequent calibration. [Pg.163]


See other pages where Band position is mentioned: [Pg.2205]    [Pg.22]    [Pg.207]    [Pg.200]    [Pg.447]    [Pg.18]    [Pg.721]    [Pg.511]    [Pg.82]    [Pg.242]    [Pg.99]    [Pg.478]    [Pg.201]    [Pg.219]    [Pg.241]    [Pg.259]    [Pg.275]    [Pg.31]    [Pg.34]    [Pg.444]    [Pg.461]    [Pg.363]    [Pg.98]    [Pg.150]    [Pg.159]    [Pg.163]    [Pg.1012]    [Pg.180]    [Pg.414]    [Pg.47]    [Pg.48]    [Pg.108]    [Pg.277]    [Pg.122]    [Pg.123]   
See also in sourсe #XX -- [ Pg.139 ]

See also in sourсe #XX -- [ Pg.4 , Pg.251 ]

See also in sourсe #XX -- [ Pg.139 ]




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Absorption bands position in relation to structures

Amides infrared absorption band positions

Band edge position

Band energy position

Band positions calculation

Band positions carbonate

Band positions cellulose

Band positions combination

Band positions overtone

Band positions polymers

Band-gap positions

Carboxylic acids infrared absorption band positions

Flatband Potential and Position of Energy Bands at the Interface

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Shifts in band positions

Surface band position

The Influence of Isotopic Substitution on Band Position

The Position of Absorption Bands

Valence band energetic positions

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