2013
DOI: 10.2138/am.2013.4349
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In situ Raman spectroscopic study of transient polyhedral distortions during cesium ion exchange into sitinakite

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Cited by 16 publications
(19 citation statements)
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“…Weak bands at 714 and 716 cm −1 observed for ivanyukite-Na- C and Cu-rich ivanyukite-K may be attributed to the hydroxyl deformation (librational) mode (Frost and Kloprogge, 2003; Seki et al , 2020). The most intense bands at 595 and 599 cm −1 for rhombohedral and cubic ivanyukite-Na are significantly shifted (by ~60 cm −1 ) in comparison with the band at 533 cm −1 observed in the spectrum of Cu-rich ivanyukite-K and are related to the asymmetric bending vibrations of Si‒O bonds or overlapping stretching vibrations of Ti‒O bonds (Filippi et al , 2007; Celestian et al , 2013). This band also can be due to Cu−O stretching vibrations of mixed Cu−O−Ti stretching vibrations involving a Cu−O3 bond.…”
Section: Raman Spectroscopymentioning
confidence: 99%
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“…Weak bands at 714 and 716 cm −1 observed for ivanyukite-Na- C and Cu-rich ivanyukite-K may be attributed to the hydroxyl deformation (librational) mode (Frost and Kloprogge, 2003; Seki et al , 2020). The most intense bands at 595 and 599 cm −1 for rhombohedral and cubic ivanyukite-Na are significantly shifted (by ~60 cm −1 ) in comparison with the band at 533 cm −1 observed in the spectrum of Cu-rich ivanyukite-K and are related to the asymmetric bending vibrations of Si‒O bonds or overlapping stretching vibrations of Ti‒O bonds (Filippi et al , 2007; Celestian et al , 2013). This band also can be due to Cu−O stretching vibrations of mixed Cu−O−Ti stretching vibrations involving a Cu−O3 bond.…”
Section: Raman Spectroscopymentioning
confidence: 99%
“…The spectrum of cubic Cu-rich ivanyukite-K is similar to that of pharmacosiderite from Cornwall, England, taken from sample R050574 of the RRUFF project (Lafuente et al , 2015). The assignments of the absorption bands were made by analogy with structurally related pharmacosiderite (Frost and Kloprogge, 2003; Filippi, 2004; Filippi et al , 2007) and titanosilicates (Celestian et al , 2013; Pakhomovsky et al , 2018; Yakovenchuk et al , 2019) and are given in Table 2.
Fig.
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Section: Raman Spectroscopymentioning
confidence: 99%
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“…The band at 687 and weak band at 792 cm −1 are related to the symmetric stretching vibrations of the same bonds (Yakovenchuk et al , 2019). The most intense band at 597 cm −1 is related to the asymmetric bending vibrations of Si‒O bonds or overlapping stretching vibrations of Ti‒O bonds (Filippi et al , 2007; Celestian et al , 2013). The bands in the range 350‒500 cm −1 correspond to symmetric bending vibrations of O‒Si‒O bonds and overlapping stretching vibrations of Ti‒O bonds (Filippi et al , 2007; Pakhomovsky et al , 2018; Yakovenchuk et al , 2019).…”
Section: Resultsmentioning
confidence: 99%
“…Data pertaining to absorption strength, peak shape, position, and assignment of the bands in both the FTIR and Raman spectra are given in Tables 2a and 2b, respectively. Absorption bands were initially identified using data from Farmer (1974); specific assignments of those bands involving Ti-O-Si chains were made using data provided by Celestian et al (2013) for synthetic sitinakite, HNa 2 KTi 4 Si 2 O 14 ·4H 2 O, whose Raman spectrum is very similar to that of hogarthite. In general, the two vibrational spectra for hogarthite are quite similar to one another, such that absorption bands in both spectra can be discussed in terms of four major groupings: (1) bands at >3000 cm -1 ; (2) bands between 700 and 1200 cm -1 ; (3) bands between 400 and 700 cm -1 ; and (4) bands …”
Section: Infrared and Raman Analysesmentioning
confidence: 99%