Abstract

The timing of carving of Grand Canyon has been debated for over 100 years with competing endmember hypotheses advocating for either a 70 Ma (“old”) or <6 Ma (“young”) Grand Canyon. Several geological constraints appear to support a “young” canyon model, but thermochronometric measures of cooling history and corresponding estimates of landscape evolution have been in debate. In particular, 4He/3He thermochronometric data record the distribution of radiogenic 4He (from the 238U, 235U and 232Th decay series) within an individual apatite crystal and thus are highly sensitive to the thermal history corresponding to landscape evolution. However, there are several complicating factors that make interpreting such data challenging in geologic scenarios involving reheating. Here, we analyze new data that provide measures of the cooling of basement rocks at the base of westernmost Grand Canyon, and use these data as a testbed for exploring the resolving power and limitations of 4He/3He data in general. We explore a range of thermal histories and find that these data are most consistent with a “young” Grand Canyon. A problem with the recovered thermal history, however, is that burial temperatures are under predicted based on sedimentological evidence. A solution to this problem is to increase the resistance of alpha recoil damage to annealing, thus modifying He diffusion kinetics, allowing for higher temperatures throughout the thermal history. This limitation in quantifying radiation damage (and hence crystal retentivity) introduces non-uniqueness to interpreting time–temperature paths in rocks that resided in the apatite helium partial retention zone for long durations. Another source of non-uniqueness, is due to unknown U and Th distributions within crystals. We show that for highly zoned with a decrease in effective U of 20 ppm over the outer 80% of the radius of the crystal, the 4He/3He data could be consistent with an “old” canyon model. To reduce this non-uniqueness, we obtain U and Th zonation information for separate crystals from the same rock sample through LA-ICP-MS analysis. The observed U and Th distributions are relatively uniform and not strongly zoned, thus supporting a “young” canyon model interpretation of the 4He/3He data. Furthermore, we show that for the mapped zonation, the difference between predicted 4He/3He data for a uniform crystal and a 3D model of the crystal are minimal, highlighting that zonation is unlikely to lead us to falsely infer an “old” Grand Canyon.

Highlights

  • The origin of Grand Canyon has been the subject of debate since the first workers attempted to understand this spectacular landform (e.g. Powell, 1879; Davis, 1901)

  • Low-temperature thermochronometry is based on the temperature dependent retentivity of daughter products of radioactive decay that are sensitive to relatively low temperatures

  • We can address the general question: what geomorphic scenarios can be excluded using high precision thermochronometric data? Here, we present a numerical analysis of apatite 4He/3He data (Winn et al, 2017) in terms of permissible time–temperature paths, and explore the possibility that much of the signal can be explained by changing the U and Th zonation of the crystal

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Summary

Introduction

The origin of Grand Canyon has been the subject of debate since the first workers attempted to understand this spectacular landform (e.g. Powell, 1879; Davis, 1901). Low-temperature thermochronometry is based on the temperature dependent retentivity of daughter products of radioactive decay that are sensitive to relatively low temperatures ( nearsurface depths) This approach has been extensively applied to resolve debate surrounding Grand Canyon incision. For Grand Canyon, apatite (U–Th)/He ages predicted for multiple time–temperature paths help understand the incision history (e.g., Flowers et al, 2008; Flowers and Farley, 2012; Wernicke, 2011; Lee et al, 2013; Karlstrom et al, 2014, 2016) These inferred time–temperature paths are non-unique, and our knowledge of the He diffusion kinetics in apatite fundamentally limits their accuracy

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