Abstract

Earthquakes at lower crustal depths are common during continental collision. However, the coseismic weakening mechanisms required to propagate an earthquake at high pressures are poorly understood. Transient high-pressure fluids or melts have been proposed as a viable mechanism, but verifying this requires direct in situ measurement of fluid or melt overpressure along fault planes that have hosted dynamic ruptures. Here, we report direct measurement of highly overpressurized frictional melts along a seismic fault surface. Using Raman spectroscopy, we identified high-pressure quartz inclusions sealed in dendritic garnets that grew from frictional melts formed by lower crustal earthquakes in the Bergen Arcs, Western Norway. Melt pressure was estimated to be 1.8–2.3 GPa on the basis of an elastic model for the quartz-in-garnet system. This is ~0.5 GPa higher than the pressure recorded by the surrounding pseudotachylyte matrix and wall rocks. The recorded melt pressure could not arise solely from the volume expansion of melting, and we propose that it was generated when melt pressure approached the maximum principal stress in a system subject to high differential stress. The associated palaeostress field demonstrates that a strong lower crust accommodated up to 1 GPa differential stress during the compressive stage of the Caledonian orogeny.

Highlights

  • Earthquakes at lower crustal depths are common during continental collision

  • Field and microstructural evidence suggest that lower crustal pseudotachylytes are generated by earthquake slip in dry rocks, possibly reflecting gigapascal-level differential stress[7,8,9]

  • Transient high fluid or melt pressures generated due to localized shearing has been proposed as a likely cause of weakening[11], but so far it has not been possible to constrain the pressure of the frictional melt during slip directly from observations of pseudotachylytes or other fault zone rocks

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Summary

H19 Minimal melt P

Fully entrapped, isolated quartz inclusions (2–4 μm in diameter) situated at least 10 μm away from each other and the thin-section surface (Supplementary Fig. 4). Assuming that the dendritic garnets were fully crystallized and had gained their plastic strength after tens of seconds to a few minutes, the melt pressure estimate based on the residual quartz inclusions pressure is constrained to ~2.0–2.3 GPa for A17 and ~1.8–2.0 GPa for H19 (Fig. 2c) This pressure represents the most conservative estimate as the melt temperature cannot be lower than the ambient wall-rock temperature. Our observations demonstrate that injection veins may form due to highly pressurized frictional melts rather than dynamic tension parallel to the fault (compare Rowe et al.[13]) This may potentially provide a mechanism for coseismic fault weakening in systems subject to high differential stresses and is relevant to explain unstable slip at lower crustal conditions. Received: 12 November 2019; Accepted: 27 April 2021; Published online: 17 June 2021

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