1982
DOI: 10.1039/c39820001413
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Uses of i.r. spectroscopy in identifying ZSM zeolite structure

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Cited by 286 publications
(151 citation statements)
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“…The absorption bands at 1225, 1150-1050, 800, and 450 cm -1 are typical of highly siliceous materials. These absorptions bands have been assigned to the external asymmetric stretching, internal asymmetric stretching, external symmetric stretching and the bending modes of the Si(Al)O 4 tetrahedra, respectively [16]. A characteristic band at 550 cm -1 due to the asymmetric stretching mode in double-ring blocks is observed in each of the samples [17,18], which confirms that all the samples have the MFI structure.…”
Section: Composition and Structurementioning
confidence: 73%
“…The absorption bands at 1225, 1150-1050, 800, and 450 cm -1 are typical of highly siliceous materials. These absorptions bands have been assigned to the external asymmetric stretching, internal asymmetric stretching, external symmetric stretching and the bending modes of the Si(Al)O 4 tetrahedra, respectively [16]. A characteristic band at 550 cm -1 due to the asymmetric stretching mode in double-ring blocks is observed in each of the samples [17,18], which confirms that all the samples have the MFI structure.…”
Section: Composition and Structurementioning
confidence: 73%
“…[19] On the other hand, crystalline Si-O networks, both dense and porous silica structures, are unambiguously distinguishable from amorphous silica by the presence of an IR peak near 1230 cm À1 . [5,7,14,20,21] This peak is indicative of the presence of translational symmetry in the silicon-oxygen network and therefore may serve as an even better indicator for the existence of zeolite subnanoparticles when other crystalline dense silica phases are not present. This is especially important for analyzing zeolite films.…”
mentioning
confidence: 96%
“…Analysis of the range 400-650 cm À1 clearly shows the presence of the peak near 550 cm À1 which is the commonly used indicator for the silicalite-1 structure. [14] So far, the small peak near 625 cm À1 in the spectra of the as-made samples has not been discussed in detail in the literature, because in transmittance IR spectra it overlaps with the much stronger peak at 550 cm À1 and appears only as a shoulder. The peak broadening observed for the spin-coated films can be due to several factors: 1) phonon confinement effects; the small size of the particles suggests a strong impact of particle-particle interaction on the bulk phonons due to the close particle packing in the formed film; 2) possible partial damage of the zeolite subnanoparticles during the coating procedure; and 3) deposition of subnanoparticles with both well-developed and poor MFI structures from the clear TEOS-CTAB solution.…”
mentioning
confidence: 97%
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