2017
DOI: 10.1016/j.saa.2017.05.046
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In-situ studies on the micro-structure evolution of A 2 W 2 O 7 (A = Li, Na, K) during melting by high temperature Raman spectroscopy and density functional theory

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Cited by 18 publications
(16 citation statements)
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“…Research showed that [ 27,58 ] different kinds of cation have delicate effects on the characteristic wavenumber of the symmetric stretching vibration mode of W–O nb in melts, which should not be neglected. The characteristic symmetric stretching vibration wavenumbers and Raman scattering activity of W–O nb bonds of single molecule A 2 W 2 O 7 (A = Li, Na, and K) model clusters were calculated along with their bond lengths in our previous work, [ 23 ] which confirmed that the average bond length of W–O nb in the W–O model clusters increases in the order of Li + , Na + , and K + . The longer the average bond length of W–O nb , the lower the characteristic wavenumber of W–O nb symmetric stretching vibration mode.…”
Section: Resultssupporting
confidence: 60%
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“…Research showed that [ 27,58 ] different kinds of cation have delicate effects on the characteristic wavenumber of the symmetric stretching vibration mode of W–O nb in melts, which should not be neglected. The characteristic symmetric stretching vibration wavenumbers and Raman scattering activity of W–O nb bonds of single molecule A 2 W 2 O 7 (A = Li, Na, and K) model clusters were calculated along with their bond lengths in our previous work, [ 23 ] which confirmed that the average bond length of W–O nb in the W–O model clusters increases in the order of Li + , Na + , and K + . The longer the average bond length of W–O nb , the lower the characteristic wavenumber of W–O nb symmetric stretching vibration mode.…”
Section: Resultssupporting
confidence: 60%
“…In order to eliminate the anharmonic effect [ 56,57 ] induced by high temperatures, all samples are compared at the same temperature of 1273 K. Based on our experiments, the W–O nb characteristic symmetric stretching vibration wavenumbers of the four‐coordinated W–O complex vary with melt compositions A 2 W n O 3n + 1 as shown in Figure 4. The corresponding major W–O complex existing in melt stably is the isolated [WO 4 ] 2− ( Q 0 ), [ 27 ] [W 2 O 7 ] 2− dimer (2 Q11), [ 23,24,29 ] and [W 3 O 10 ] 2− trimer ( 2Q12 and Q211), [ 30–32 ] respectively, for n values of 1, 2, and 3. This is consistent with the trend shown in Figure 2, namely, v ( Q 0 ) < v ( Q11) < v ( Q12) < v ( Q211).…”
Section: Resultsmentioning
confidence: 99%
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“…Previous studies have demonstrated that Raman scattering spectroscopy is a feasible and informative tool for investigating the phase transformation of tungstates and probing the structure of W–O complexes in crystalline, glassy, and molten states. The relative intensities show the variation in the relative amount of each species.…”
Section: Introductionmentioning
confidence: 99%
“…The in situ HTRS and DFT methods further improved the structure information of W–O complexes in the crystal, melt, and solid–liquid phase transitions, which is beneficial to the optimization of the conditions of crystal growth from melt for tungstate functional crystals. 145 Furthermore, they investigated the Raman spectra of sodium disilicate crystal, glass, and its melt structure. The Raman spectra of Na 2 Si 2 O 5 from room temperature to 1773 K was measured in solid and liquid states, and the temperature-dependent variations of the structure units were analyzed.…”
Section: Introductionmentioning
confidence: 99%