Mineral host-inclusion systems preserve crucial information regarding their geologic history. For example, we can determine their pressure and temperature of formation with elastic geobarometry. It is possible to determine the strain of the inclusion when still entrapped in its host by measuring changes in the Raman peak positions from those of a free crystal, which are interpreted through the inclusion phonon-mode Grüneisen tensors (Grüneisen 1926). The calculated inclusion strains can then be used in an elastic model to back-calculate the pressure and temperature conditions of entrapment.
While this approach works for many host-inclusion systems (e.g., quartz or zircon in garnet), there remain several challenges. For example, when both the host and the inclusion are anisotropic, symmetry-breaking strains are generally developed within the inclusion and change the Raman peak positions, and this can lead to errors in the calculation of the inclusion strains and pressure and hence their entrapment conditions (Murri et al. 2022). Many common inclusions are solid solutions (e.g., clinopyroxenes, apatites) in which the positions of the Raman modes change as a function of their chemical composition and cation ordering. These changes must be determined before using Raman modes to determine the inclusion pressure (Baratelli et al. 2024). The thermoelastic properties of minerals also depend on their composition, so one has to know how the EoS of both the host and the inclusion depend on their composition to correctly calculate entrapment conditions (e.g., garnet solid solutions, Angel et al. 2022). The interpretation of inclusion pressures in terms of the geological history of the rock also depends on whether the inclusion stress has been reset following entrapment; for some host-inclusion systems, such as zircon in garnet, resetting is so fast on a laboratory timescale (Campomenosi et al. 2023) that measured inclusion pressures can reflect not the original entrapment, but a point on the exhumation path (Campomenosi et al. 2021).
References:
Angel, R. J., Gilio, M., Mazzucchelli, M., & Alvaro, M., 2022. Contributions to Mineralogy and Petrology, 177(5), 54.
Baratelli, L., Murri, M., Alvaro, M., Prencipe, M., Mihailova, B., & Cámara, F., 2024. American Mineralogist: Journal of Earth and Planetary Materials.
Campomenosi, N., Scambelluri, M., Angel, R. J., Hermann, J., Mazzucchelli, M. L., Mihailova, B., ... & Alvaro, M., 2021. Contributions to Mineralogy and Petrology, 176, 1-17.
Campomenosi, N., Angel, R. J., Alvaro, M., & Mihailova, B., 2023. Geology, 51(1), 23-27.
Grüneisen, E., 1926. Zustand des festen K¨orpers. Handbuch der Physik 1, 1–52
Murri, M., Gonzalez, J. P., Mazzucchelli, M. L., Prencipe, M., Mihailova, B., Angel, R. J., & Alvaro, M., 2022. Lithos, 422, 106716.