The Raman spectra of Ca1-xSrxAl2Si2O8 (0 ≤ x ≤ 1) feldspars have been measured, to investigate at a short-range scale the effect of changing composition on the P (Formula presented.) ➔ I (Formula presented.) and I (Formula presented.) ➔ I2/c phase transitions and how phase transitions affect the mechano-luminescence found in these feldspars. Transmission electron microscopy (TEM) and X-ray diffraction (XRD) were done on the same samples, to pinpoint the transitions, by the analysis of selected area diffraction patterns (SAED) and of the spontaneous strain. Natural anorthite (CaAl2Si2O8) shows a large number of well-resolved peaks, together with sharp h + k even, l odd diffractions (c-type) in SAED patterns, indicative of a P (Formula presented.) symmetry. In synthetic anorthite, the Raman spectrum is similar to that of natural anorthite, but the peaks are broader, and c-type reflections are elongated. As Sr increases, the c-type reflections become more diffuse and elongated, as the Raman peaks do. At x > 0.6, new peaks appear in Raman spectra, and other peaks show a change in their wavenumber. Moreover, the c-type reflections disappear completely, and the lattice becomes I-centred. Between x ~ 0.6 and x = 0.86(3), the XRD patterns prompt for a triclinic structure, with S.G. I (Formula presented.). The transition to the monoclinic I2/c structure is well constrained by the ferroelastic strain, whereas the Raman spectra are more similar between the monoclinic and triclinic I (Formula presented.) and I2/c than between I (Formula presented.) and P (Formula presented.). The absence of mechano-luminescence in triclinic I (Formula presented.) compositions suggests that this property is enhanced in local P (Formula presented.) configurations at conditions close to the P (Formula presented.) to I (Formula presented.) transition. A possible mechanism for mechano-luminescence involving a compression induced P (Formula presented.) to I (Formula presented.) transition in local Eu2+ bearing P (Formula presented.) configurations is proposed.
Raman spectroscopy, phase transitions, microstructures, and mechano-luminescence in Ca-Sr feldspars (CaAl2Si2O8-SrAl2Si2O8)
Curetti N.;Bernasconi D.;Tribaudino M.
Membro del Collaboration Group
2024-01-01
Abstract
The Raman spectra of Ca1-xSrxAl2Si2O8 (0 ≤ x ≤ 1) feldspars have been measured, to investigate at a short-range scale the effect of changing composition on the P (Formula presented.) ➔ I (Formula presented.) and I (Formula presented.) ➔ I2/c phase transitions and how phase transitions affect the mechano-luminescence found in these feldspars. Transmission electron microscopy (TEM) and X-ray diffraction (XRD) were done on the same samples, to pinpoint the transitions, by the analysis of selected area diffraction patterns (SAED) and of the spontaneous strain. Natural anorthite (CaAl2Si2O8) shows a large number of well-resolved peaks, together with sharp h + k even, l odd diffractions (c-type) in SAED patterns, indicative of a P (Formula presented.) symmetry. In synthetic anorthite, the Raman spectrum is similar to that of natural anorthite, but the peaks are broader, and c-type reflections are elongated. As Sr increases, the c-type reflections become more diffuse and elongated, as the Raman peaks do. At x > 0.6, new peaks appear in Raman spectra, and other peaks show a change in their wavenumber. Moreover, the c-type reflections disappear completely, and the lattice becomes I-centred. Between x ~ 0.6 and x = 0.86(3), the XRD patterns prompt for a triclinic structure, with S.G. I (Formula presented.). The transition to the monoclinic I2/c structure is well constrained by the ferroelastic strain, whereas the Raman spectra are more similar between the monoclinic and triclinic I (Formula presented.) and I2/c than between I (Formula presented.) and P (Formula presented.). The absence of mechano-luminescence in triclinic I (Formula presented.) compositions suggests that this property is enhanced in local P (Formula presented.) configurations at conditions close to the P (Formula presented.) to I (Formula presented.) transition. A possible mechanism for mechano-luminescence involving a compression induced P (Formula presented.) to I (Formula presented.) transition in local Eu2+ bearing P (Formula presented.) configurations is proposed.File | Dimensione | Formato | |
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