美国大峡谷大不整合地层的深时热历史:锆石(U-Th)/He 和 K 长石 40Ar/39Ar 热时计组合

O.G. Thurston, W.R. Guenthner, K.E. Karlstrom, M. Heizler, J.W. Ricketts, K.T. McDannell
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摘要

通过锆石(U-Th)/氦(ZHe)方法进行的深时热年代学研究是一个新兴的研究领域,有望对前寒武纪岩石热和剥蚀历史进行约束。大峡谷为进一步探索这种方法提供了机会,因为出色的地质制约因素可以与多个热时计相结合,以解决有关亚寒武纪大不整合复合侵蚀面下基底侵蚀空间变异性的重要问题。在这项研究中,我们综合了来自美国大峡谷前寒武纪基底岩石的新 ZHe 结果(n = 26)和已发表的(n = 77)ZHe 数据,以及新的 K 长石 40Ar/39Ar 数据和模型(n = 4)。我们使用 HeFTy 和 QTQt 热历史建模来评估单个 ZHe 和 K 长石 40Ar/39Ar 热年代测定数据集解析前寒武纪热历史的能力,并将这些结果与使用 QTQt 软件联合建模的数据进行比较。我们还比较了大峡谷东部和西部的前寒武纪基底热历史,大峡谷东部有 4 公里的大峡谷超群地层沉积并保存下来,而大峡谷西部的超群地层要么从未沉积,要么没有保存下来。在所有地点,与结合长石 40Ar/39Ar 和 ZHe 数据的模型相比,仅受 ZHe 数据约束的模型对过去 ∼600 m.y. 的解析能力有限,而结合长石 40Ar/39Ar 和 ZHe 数据的模型可将记录的历史延伸到中新生代。我们的模型结果表明,发生了两次区域性基底揭顶事件。约 1350-1250 Ma 的冷却事件被解释为记录了基底从 ∼ 10 km 深处的掘出,而第二次冷却事件(总计 ∼ 200-100 °C)记录了从 ∼ 3 km 至 7 km 深处的掘出,到约 600-Ma 至 500-Ma 之间的近地表条件。大峡谷最东部的模型表明,大峡谷超群保存下来的最大厚度为 4 公里(埋藏加热温度为 100 °C),接近中新生代和新近纪地层的原始总厚度。至于这些超基性岩是否如区域地质研究结果所表明的那样,在大峡谷西部存在过,然后被侵蚀,还是从未沉积过,热年代学数据并没有给出确切的结论。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Deep-time thermal history of the Great Unconformity in the Grand Canyon, USA: Combined zircon (U-Th)/He and K-feldspar 40Ar/39Ar thermochronometers
Deep-time thermochronology by the zircon (U-Th)/He (ZHe) method is an emerging field of study with promise for constraining Precambrian rock thermal and exhumation histories. The Grand Canyon provides an opportunity to further explore this method because excellent geologic constraints can be integrated with multiple thermochronometers to address important questions about the spatial variability of basement erosion below the sub-Cambrian Great Unconformity composite erosional surface. In this study, we synthesize new ZHe results (n = 26) and published (n = 77) ZHe data with new K-feldspar 40Ar/39Ar data and models (n = 4) from Precambrian basement rocks of the Grand Canyon, USA. We use HeFTy and QTQt thermal history modeling to evaluate the ability of the individual ZHe and K-feldspar 40Ar/39Ar thermochronometric data sets to resolve Precambrian thermal histories and compare those results with jointly modeled data using the QTQt software. We also compare Precambrian basement thermal histories of the eastern and western Grand Canyon, where the eastern Grand Canyon has ∼4 km of Grand Canyon Supergroup strata deposited and preserved, and the western Grand Canyon, where the Supergroup was either never deposited or not preserved. In all locations, models constrained only by ZHe data have limited resolving power for the past ∼600 m.y., compared to models that combine K-feldspar 40Ar/39Ar and ZHe data, which extends the recorded history into the Mesoproterozoic. Our model results suggest that two regional basement unroofing events occurred. A ca. 1350−1250 Ma cooling event is interpreted to record basement exhumation from depths of ∼10 km, and a second cooling episode (∼200−100 °C total) records exhumation from a depth of ∼3 km to 7 km to near-surface conditions between ca. 600 Ma and 500 Ma. Easternmost Grand Canyon models suggest that the preserved maximum ∼4 km thickness of the Grand Canyon Supergroup (with burial heating at ∼100 °C) approximates the total original Mesoproterozoic and Neoproterozoic stratal thickness. Whether these Supergroup rocks were present and then eroded in the western Grand Canyon, as suggested by regional geologic studies, or were never deposited is not constrained by thermochronological data.
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