Abstract Extreme grain-size reduction due to cataclasis, neocrystallization or phase change results in a switch to diffusion creep and dramatic weakening in deforming rocks. Grain growth increases strength until dislocation creep becomes a significant deformation mechanism. We quantify the ‘lifetime’ of diffusion creep by substituting the normal grain growth law into the diffusion creep flow law to calculate the time taken for dislocation creep to become significant. Stress-temperature and strain-rate-temperature space is outlined where diffusion creep may accommodate significant strain: these regions have an upper temperature limit beyond which grain growth is fast enough to move the rock quickly into the dislocation creep field. For plagioclase the limit lies in the amphibolite facies. Rocks in a mantle upwelling experience grain-size reduction during phase changes. Pressure-dependent grain growth limits the deformation that can be accommodated by diffusion creep. This time limit and associated strain limit is independent of starting grain size with a small dependence on upwelling rate and plume width. In both these tectonic environments, second phases are likely to play a role in the maximum achievable grain size due to grain-boundary pinning. Hence we predict the minimum lifetimes of diffusion-creep-dominated deformation following extreme grain-size reduction.

Abstract The Lewisian Complex is an Archaean-Proterozoic high-grade gneiss region with widespread amphibolite-facies fabrics. These fabrics have, on the 100 km scale, a subhorizontal enveloping surface and are interpreted as forming in gently dipping crustal-scale shear zones and steeper lateral ramp structures. The Scourie dyke swarm, of Proterozoic age, runs NW-SE subvertically outside such zones, but is transformed into subhorizontal concordant amphibolite sheets within them. The terms ‘Scourian’ and ‘Laxfordian’ are used to describe pre-dyke and post-dyke fabrics and events. In the southern mainland Lewisian at Loch Torridon, unmodified Scourian gneisses in the north pass southwards into lozenges bounded by anastomosing zones of Laxfordian deformation, and eventually to a region consisting entirely of Laxfordian fabrics. This geometry is compatible with a major Laxfordian shear zone that dips northeastwards beneath a Scourian hanging wall. Detailed maps show that structures on the metre to kilometre scale do not relate in a simple way to the crustal shear zone model for four reasons. First, many amphibolite-facies fabrics in the quartzo-feldspathic gneisses predate the dykes (they relate to a late Scourian or ‘Inverian’ event), so the dykes cannot be used to infer overall geometry and movement sense. A few structures along the Loch Roag Line, the most northeasterly high-strain belt in the Loch Torridon inliers, may indicate syntectonic dyke emplacement. Second, local shear with opposing senses is present in both the pre-dyke and post-dyke (Laxfordian) deformation. Third, foliation deflections on a variety of scales relate more to varying shear planes than to the deflection caused by increasing simple shear strain, and cannot be used to infer shear sense. Fourth, there is pure-shear stretching within the gneisses that masks the effects of simple shear. These structures can be incorporated into a crustal-scale shear zone model, but are not diagnostic of it. The scatter of foliation planes with a relatively constant lineation is a feature of other crustal-scale high-strain zones (e.g. Canisp, Nordre Strømfjord), although different explanations are available. Other high-strain zones (e.g. the Laxford Front) show a spatially varying lineation pattern, but this could relate more to a varying shear direction than to deflections of linear features into a single movement direction. The geometry of classic simple shear is not versatile enough to explain the kilometre-scale geometry of such high-strain zone, although it may work well in local subareas.