Abstract
Synthetic thorite and huttonite, two polymorphs of ThSiO4, were investigated by a combination of in situ high-pressure synchrotron X-ray powder diffraction and in situ high-pressure Raman spectroscopy. The average onset pressure of the thorite-to-huttonite transition was determined to be 6.6 ± 0.2 GPa, using both techniques. The bulk moduli of thorite and huttonite were determined to be 139(9) and 246(11) GPa, respectively, by fitting their unit-cell volume data to a second-order Birch-Murnaghan equation of state (EOS). Based on its bulk modulus, thorite is the most compressible zircon-structured orthosilicate, as it has the largest unit-cell volume among tetravalent metal orthosilicates. The pressure derivatives of the vibrational modes of thorite were found to be consistent with those previously reported for other orthosilicates (e.g., zircon, hafnon, stetindite, and coffinite), while having the smallest Grüneisen parameter. A new P-T phase diagram for ThSiO4 is proposed, where the boundary of the thorite →huttonite transition is: P(T) = (7.8 ± 0.9 GPa) – (0.006 ± 0.002 GPa/K)T. Based on the new P-T phase diagram, we further estimated the enthalpy of formation of huttonite, ΔH f,ox, to be 0.6± 6.0 kJ/mol, suggesting its metastability and rare locality in nature.
| Original language | English |
|---|---|
| Pages (from-to) | 1428-1436 |
| Number of pages | 9 |
| Journal | American Mineralogist |
| Volume | 110 |
| Issue number | 9 |
| DOIs | |
| State | Published - Sep 1 2025 |
Funding
This work was supported by the institutional funds from the Department of Chemistry at Washington State University in the early stage and later supported by the National Science Foundation (NSF), Division of Earth Sciences, under award no. 2149848, and Division of Materials Research, under award no. 2144792. We also acknowledge the help from the Alexandra Navrotsky Institute for Experimental Thermodynamics, and the WSU-PNNL Nuclear Science and Technology Institute. Research presented in this article was supported by the Laboratory Directed Research and Development (LDRD) program of Los Alamos National Laboratory (LANL) under project number 20180007DR. LANL, an affirmative action/equal opportunity employer, is managed by Triad National Security, LLC, for the National Nuclear Security Administration of the U.S. Department of Energy under contract 89233218CNA000001. A portion of this work was performed at GeoSoilEnviroCARS (The University of Chicago, Sector 13), Advanced Photon Source (APS), Argonne National Laboratory. GeoSoilEnviroCARS is supported by the NSF–Earth Sciences (EAR-1634415). This research used resources of the Advanced Photon Source, a U.S. Department of Energy (DOE) Office of Science User Facility operated for the DOE Office of Science by Argonne National Laboratory under Contract No. DE-AC02-06CH11357. This work was supported by the institutional funds from the Department ofChemistry at Washington State University in the early stage and later supportedbythe NationalScienceFoundation (NSF),DivisionofEarthSciences, underawardno. 2149848, and Division of Materials Research, under award no. 2144792. Wealso acknowledgethe help from the Alexandra Navrotsky Institute for ExperimentalThermodynamics, and the WSU-PNNL Nuclear Science and Technology Institute.Research presented in this article was supported by the Laboratory DirectedResearch and Development (LDRD) program of Los Alamos National Laboratory(LANL) under project number 20180007DR. LANL, an affirmative action/equalopportunity employer,ismanagedbyTriadNationalSecurity,LLC,forthe NationalNuclear Security Administration of the U.S. Department of Energy under contract89233218CNA000001. A portion of this work was performed at GeoSoilEnviroCARS (The University of Chicago, Sector 13), Advanced Photon Source (APS),ArgonneNational Laboratory. GeoSoilEnviroCARSissupportedbythe NSF–EarthSciences (EAR-1634415). This research used resources of the Advanced PhotonSource, a U.S. Department of Energy (DOE) Office of Science User Facility operated for the DOEOffice ofSciencebyArgonne National Laboratoryunder ContractNo. DE-AC02-06CH11357
Keywords
- Thorite
- X-ray diffraction
- equation of state
- high pressure
- huttonite
- metastability
- phase diagram