Answers are grounded in this paper and cite their sources.
Synchrotron radiation B K-edge XANES spectra are reported for 19 borate and borosilicate minerals. The spectra are characterized by three prominent features; a sharp peak (A) at ~194 eV (the edge feature of trigonal B; III B), a broader peak (B) at 197-199 eV (the edge feature of tetrahedral B, IV B), and a broad peak (C) at 200-201 eV for tetrahedral B and 203-204 eV for trigonal B. The area of peak A is very sensitive to content of III B and its position yields information on B-O bond length and linkage of the BO 3 group. The area of peak B is proportional to content of IV B but quantification is limited by overlap with peak C. The width of peak B increases with increasing divergence of B-O bond lengths, responding to splitting of σ*(t 2 ) antibonding orbitals. The tetrahedral component of peak C appears to be a s-shape resonance. For trigonal B minerals, the relative intensity of peak C and its satellite peaks increases with increase in mean size and/or atomic number of next-nearestneighbor cations, C being most intense in vonsenite (Fe 2 Fe 3+ BO 5 ). Priceite (Ca 4 B 10 O 19 ·7H 2 O), of unknown structure, has 80% IV B, and an isolated BX3 group with III B-O = 1.373(5) Å. Comparison of B K-edge XANES spectra collected using total electron yield (sampling depth <60 Å) and fluorescence yield (sampling depth <1100 Å) shows that borates and borosilicates readily reconstruct in surface and near-surface environments. More profound structural damage involving conversion of IV B to III B occurs in minerals with high contents of IV B, and hydrous Mg borates with interstitial H 2 O are unstable in the high vacuum of the spectrometer.
No takes yet. Share an insight, caveat, or question.
Fleet et al. (2000) studied this question.
Synapse has enriched 10 related papers. Consider them for comparative context: