PHASE-RELATIONS IN NA2O-SIO2 AND K2SI4O9 SYSTEMS UP TO 14 GPA AND SI-29 NMR-STUDY OF THE NEW HIGH-PRESSURE PHASES - IMPLICATIONS TO THE STRUCTURE OF HIGH-PRESSURE SILICATE-GLASSES
M. Kanzaki et al., PHASE-RELATIONS IN NA2O-SIO2 AND K2SI4O9 SYSTEMS UP TO 14 GPA AND SI-29 NMR-STUDY OF THE NEW HIGH-PRESSURE PHASES - IMPLICATIONS TO THE STRUCTURE OF HIGH-PRESSURE SILICATE-GLASSES, Physics of the earth and planetary interiors, 107(1-3), 1998, pp. 9-21
Preliminary studies have been made of phase relations in the K2SI4O9,
Na2Si2O5, Na2Si3O7 and Na2Si4O9 systems up to 14 GPa. Several high-pre
ssure sodium silicate phases have been observed for the first time and
were characterized by means of powder X-ray diffraction and Si-29 MAS
NMR techniques; In the K2Si4O9 system, the wadeite (K2ZrSi3O9)-type p
hase was found to be stable and melt congruently at least up to 12 GPa
. In the Na2Si2O5 system, phase C, a Na2Si2O5 polymorph previously rep
orted at 10-40 MPa, was observed at 2.5 GPa. However, at 5-6 GPa, a pr
eviously unknown phase (epsilon-Na2Si2O5) appeared. This phase was rep
laced by yet another new phase(zeta-Na2Si2O5) at 8-10 GPa. In the Na2S
i3O7 system, a new high-pressure Na2Si3O7 phase was detected at about
10 GPa. In the Na2Si4O9 system, a new Na2Si3O7 phase appeared at 6-8 G
Pa and it decomposed to stishovite (SiO2) plus the high-pressure Na2Si
3O7 phase at greater than or equal to 10 GPa. The Si-29 MAS NMR spectr
a revealed that the epsilon-Na2Si2O5 phase contains only tetrahedral S
i sites, whereas the zeta-Na2Si2O5, Na2Si3O7 and Na2Si4O9 phases conta
in both tetrahedral and octahedral Si sites. Recently, Fleet and Hende
rson [Fleet, M., Henderson, G.S., 1995a. Epsilon sodium disilicate: A
high-pressure layer structure [Na2Si2O5]. J. Solid State Chem., 119: 4
00-404; Fleet, M., Henderson, G.S., 1995b. Sodium trisilicate: A new h
igh-pressure silicate structure (Na2Si[Si2O7]). Phys. Chem. Min., 22.
383-386.] and Fleet [Fleet, M., 1996. Sodium tetrasilicate: A complex
high-pressure framework silicate (Na2Si3[Si9O27]). Am. Mineral., 81. 1
105-1110.] have determined the structures of the epsilon-Na2Si2O5, Na2
Si3O7 and Na2Si4O9 phases. Subsolidus phase transformations with press
ure for these alkali silicate systems can be described in terms of red
uction of Si-O-Si angles at lower pressures and formation of octahedra
l Si through conversion of nonbridging oxygens to bridging oxygens at
higher pressures. Similar structural changes might be expected for alk
ali silicate glasses (and melts) within this pressure range. (C) 1998
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