Raman scattering continuous resonance

Figure 6.1-3 Schematic representation of continuum resonance Raman scattering for the Br2 molecule. The incident laser frequency (o o) is in resonance with the continuous states of the repulsive 77 excited state and the repulsive part of the bound B(- 77o-i- ) state, which is above the dissociation limit at around 20 000 cm (Baierl and Kiefer, 1981).

Figure 6.1-4 Illustration of Eq. 6.1-19, the time-dependent approach to continuum resonance Raman scattering. Shown is a 2 > 1> vibrational Raman transition in Bra for Aq = 457.9 nm excitation. As examples, (A), (B) and (C) show the potential curves of the relevant ground (X = continuous line) and excited (B = 7o+m, dashed line, and 77 = 7T , dotted line) electronic states, together with the absolute values of the coordinate representations of the initial state It >= 1 >, final state ]f >= 2 >, and the time-dependent state i(r) > at times / = 0, 20 and 40 fs, respectively. The excitation and de-excitation processes and the related unimolecular dissociations are indicated schematically by vertical and horizontal arrows. For clarity of presentation, the energy gap between state (> and f> is expanded (Ganz et al., 1990).

Numerous nanocomposite characterization methods are available thermogravimetric analysis (TGA), differential scanning calorimetry [DSC], transmission electron microscopy (TEM), scanning electron microscopy (SEM), X-ray diffraction (XRD), nuclear magnetic resonance (NMR), IR spectroscopy, Raman spectroscopy, X-ray photoelectron spectroscopy, dielectric relaxation spectroscopy, atomic force microscopy [AFM], electron spin resonance, continuous-wave and pulsed ESR spectroscopy and others [59]. Among all of the methods, TGA, DSC, wide-angle scattering diffraction [WAXS], and TEM are the most commonty used and will be discussed in detail. 

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