TY - JOUR
T1 - Structure and crystal-field spectra of Co3Al2(SiO4)3 and (Mg,Ni)3Al2(SiO4)3 garnet
AU - Ross, Charles R.
AU - Keppler, Hans
AU - Canil, Dante
AU - O'Neill, Hugh St C.
N1 - Copyright:
Copyright 2021 Elsevier B.V., All rights reserved.
PY - 1996
Y1 - 1996
N2 - Synthetic Co3Al2(SiO4)3 garnet and (Mg,Ni)3Al2(SiO4)3 garnet with Ni/(Ni + Mg) = 0.15-0.18 have been studied by single-crystal X-ray diffraction and optical spectroscopy. The X-ray data confirm that Co2+ and Ni2+ occupy the large distorted cubic (dodecahedral) site of the structure. Structure refinement indicates that the Ni2+ ion is probably displaced out of the center of this site and statically or dynamically disordered onto the 48g equipoint at (1/8,y,1/4+y). This is consistent with the lattice constant of the Ni-bearing garnet of 11.4717(7) Å being significantly larger than the lattice constant of pyrope (11.459 Å), although the ionic radius of Ni2+ is usually smaller than that of Mg2+. The lattice constant of Co3Al2(SiO4)3 garnet is 11.4597(2) Å. Because of the unusual coordination geometries of Ni2+ and Co2+, the optical spectra of the garnets are fundamentally different from those of other Co2+- and Ni2+-bearing silicates. The following crystal-field parameters were estimated from spectroscopic data: crystal-field splitting δ = 4430 cm-1 (Co2+) and 4210 cm-1 (Ni2+); Racah parameter B = 890 cm-1 (Co2+) and 1080 cm-1 (Ni2+). These data yield an exceptionally low crystal-field stabilization energy (CFSE) of Ni2+ in garnet of 3370 cm-1, which explains the very low Ni contents of garnets in equilibrium with olivine. The CFSE of Co2+ in garnet of 5320 cm-1 is similar to values for pyroxenes and olivine. Therefore, the partition coefficient of Co2+ between these phases should be close to unity, as is observed.
AB - Synthetic Co3Al2(SiO4)3 garnet and (Mg,Ni)3Al2(SiO4)3 garnet with Ni/(Ni + Mg) = 0.15-0.18 have been studied by single-crystal X-ray diffraction and optical spectroscopy. The X-ray data confirm that Co2+ and Ni2+ occupy the large distorted cubic (dodecahedral) site of the structure. Structure refinement indicates that the Ni2+ ion is probably displaced out of the center of this site and statically or dynamically disordered onto the 48g equipoint at (1/8,y,1/4+y). This is consistent with the lattice constant of the Ni-bearing garnet of 11.4717(7) Å being significantly larger than the lattice constant of pyrope (11.459 Å), although the ionic radius of Ni2+ is usually smaller than that of Mg2+. The lattice constant of Co3Al2(SiO4)3 garnet is 11.4597(2) Å. Because of the unusual coordination geometries of Ni2+ and Co2+, the optical spectra of the garnets are fundamentally different from those of other Co2+- and Ni2+-bearing silicates. The following crystal-field parameters were estimated from spectroscopic data: crystal-field splitting δ = 4430 cm-1 (Co2+) and 4210 cm-1 (Ni2+); Racah parameter B = 890 cm-1 (Co2+) and 1080 cm-1 (Ni2+). These data yield an exceptionally low crystal-field stabilization energy (CFSE) of Ni2+ in garnet of 3370 cm-1, which explains the very low Ni contents of garnets in equilibrium with olivine. The CFSE of Co2+ in garnet of 5320 cm-1 is similar to values for pyroxenes and olivine. Therefore, the partition coefficient of Co2+ between these phases should be close to unity, as is observed.
UR - http://www.scopus.com/inward/record.url?scp=0029770030&partnerID=8YFLogxK
U2 - 10.2138/am-1996-1-209
DO - 10.2138/am-1996-1-209
M3 - Article
AN - SCOPUS:0029770030
SN - 0003-004X
VL - 81
SP - 61
EP - 66
JO - American Mineralogist
JF - American Mineralogist
IS - 1-2
ER -