Raman Spectroscopy for Soft Matter Applications 2008
DOI: 10.1002/9780470475997.ch2
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Raman Scattering Theory and Elements of Raman Instrumentation

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Cited by 3 publications
(3 citation statements)
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“…53−56 The position of ν(M-(η 2 -O 2 )) shifts to lower wavenumbers from Ti-BEA 53 to Nb-BEA, Mo-BEA, and W-BEA 54 due to greater charge transfer from the group 6 metal center to the peroxide moiety. 57 In addition to features that appear only after contact with H 2 O 2 , spectra for Mo-and W-BEA possess a distinct feature near 970 cm −1 (Figure 2), which is attributed to ν(MO) 58,59 and is absent from spectra of Ti-BEA and Nb-BEA. Mo-BEA and W-BEA also show Raman features reminiscent of oligomeric metal oxides complexes including bridging M−O−M bonds at 700 cm −159 and 805 cm −1 for WO 3 and 880 cm −1 for MoO 3 .…”
Section: Methodssupporting
confidence: 87%
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“…53−56 The position of ν(M-(η 2 -O 2 )) shifts to lower wavenumbers from Ti-BEA 53 to Nb-BEA, Mo-BEA, and W-BEA 54 due to greater charge transfer from the group 6 metal center to the peroxide moiety. 57 In addition to features that appear only after contact with H 2 O 2 , spectra for Mo-and W-BEA possess a distinct feature near 970 cm −1 (Figure 2), which is attributed to ν(MO) 58,59 and is absent from spectra of Ti-BEA and Nb-BEA. Mo-BEA and W-BEA also show Raman features reminiscent of oligomeric metal oxides complexes including bridging M−O−M bonds at 700 cm −159 and 805 cm −1 for WO 3 and 880 cm −1 for MoO 3 .…”
Section: Methodssupporting
confidence: 87%
“…The Raman spectra of H 2 O 2 -activated Ti-, Nb-, Mo-, and W-BEA contain features between 550 and 620 cm –1 that correspond to the symmetric and asymmetric stretching modes of metal-peroxo (M-(η 2 -O 2 )) intermediates. The position of ν­(M-(η 2 -O 2 )) shifts to lower wavenumbers from Ti-BEA to Nb-BEA, Mo-BEA, and W-BEA due to greater charge transfer from the group 6 metal center to the peroxide moiety . In addition to features that appear only after contact with H 2 O 2 , spectra for Mo- and W-BEA possess a distinct feature near 970 cm –1 (Figure ), which is attributed to ν­(MO) , and is absent from spectra of Ti-BEA and Nb-BEA.…”
Section: Resultsmentioning
confidence: 99%
“…The first one was characteristic of the chemical bond at the origin of the signal, the second parameter was related to the concentration of vibrating bonds, and the last one was correlated to the disorder of the material and, especially in case of polymer, it allowed differentiating crystalline and amorphous phases. [58] In what follows we will particularly focus on two signals, the band at 1,000 cm −1 , which was common to monomer and polymer and the band at 1,631 cm −1 , which was specific to monomer (Figure 1b). We will establish quantitative relations between the characteristics of these bands and monomer conversion during emulsion polymerization.…”
Section: Resultsmentioning
confidence: 99%