Abstract

Abstract. A series of isochronal heating experiments were performed to constrain monazite fission track thermal annealing properties. The 252Cf fission tracks were implanted into monazite crystals from the Devonian Harcourt granodiorite (Victoria, Australia) on polished surfaces oriented parallel to (100) pinacoidal faces and perpendicular to the crystallographic c axis. Tracks were annealed over 1, 10, 100 and 1000 h schedules at temperatures between 30 and 400 ∘C. Track lengths were measured on captured digital image stacks and then converted to calculated mean lengths of equivalent confined fission tracks that progressively decreased with increasing temperature and time. Annealing is anisotropic, with tracks on surfaces perpendicular to the crystallographic c axis consistently annealing faster than those parallel to the (100) face. To investigate how the mean track lengths decreased as a function of annealing time and temperature, one parallel and two fanning models were fitted to the empirical dataset. The temperature limits of the monazite partial annealing zone (MPAZ) were defined as length reductions to 0.95 (lowest) and 0.5 (highest) for this study. Extrapolation of the laboratory experiments to geological timescales indicates that for a heating duration of 107 years, estimated temperature ranges of the MPAZ are −44 to 101 ∘C for the parallel model and −71 to 143 ∘C (both ±6–21 ∘C, 2 standard errors) for the best-fitting linear fanning model (T0=∞). If a monazite fission track closure temperature is approximated as the midpoint of the MPAZ, these results, for tracks with similar mass and energy distributions to those involved in spontaneous fission of 238U, are consistent with previously estimated closure temperatures (calculated from substantially higher energy particles) of < 50 ∘C and perhaps not much higher than ambient surface temperatures. Based on our findings we estimate that this closure temperature (Tc) for fission tracks in monazite ranges between ∼ 45 and 25 ∘C over geological timescales of 106–107 years, making this system potentially useful as an ultra-low-temperature thermochronometer.

Highlights

  • Fission track thermochronology is an analytical technique used to reconstruct the low-temperature thermal history of rocks over geological time

  • All length measurements are presented as mean lengths of equivalent confined fission tracks calculated according to the geometry in Fig. 3 and duplicated on surfaces oriented parallel to (100) and perpendicular to the crystallographic c axis

  • Results are averaged across both surface orientations, and the normalized track length (r = l/l0) values are calculated relative to the average length of the unannealed control samples (l0 = 10.60 μm)

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Summary

Introduction

Fission track thermochronology is an analytical technique used to reconstruct the low-temperature thermal history of rocks over geological time. Fission tracks form from the spontaneous nuclear fission of 238U, resulting in the accumulation of narrow damage trails in uranium-bearing minerals such as apatite and zircon. The time since the fission tracks began to accumulate may be calculated by measuring the spontaneous track density and uranium concentration. If the host rock experienced elevated temperatures, the fission tracks that have formed up to that point will progressively anneal and eventually disappear. Thermal diffusion drives the annealing process, with the reduction in fission track density and confined track length being a function of heating time and temperature in the host rock. From the apparent age and track length distribution, a quantitative analysis of the thermal history of the host rock can be achieved. For fundamentals of the fission track technique, including methodology and applications, see Wagner and Van den Haute (1992) and Malusa and Fitzgerald (2019)

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