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Radon loss from zircon: Effects of microstructure on radon emanation and diffusion.

机译:锆石中的loss损失:微观结构对ra散发和扩散的影响。

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摘要

Radon emanation from rocks and minerals is ubiquitous, but the mechanisms of radon loss are not well understood. Quantification of radon emanation rates from zircon has potential bearing on the reliability of U-Pb ages of zircon bearing rocks. The 238U decay chain includes 222Rn, a noble gas, which has a half-life of 3.82 days and can escape from the crystal structure of zircon if sufficient pathways exist, or by recoil if the parent 238U was very near the outer edge of the crystal. Loss of 222Rn ultimately leads to a deficiency of 206Pb, resulting in discordance between 238U-206Pb, 235U-207Pb, and 232Th-208Pb ages. In order to evaluate the factors affecting radon loss from zircon, we performed two experiments: one focused on the effect of microstructure on room temperature 222Rn emanation, and the other to investigate 222Rn loss by high temperature diffusion. Large (~100 g) single crystal zircon samples from each of three localities were selected for this study: Mud Tank, Malawi, and Bancroft. The zircons were pulverized and five grain sizes (500 mum, 250-500 mum, 125-250 mum, 63 - 125 mum, and < 63 mum) were separated from each. Room temperature radon emanation rates were measured for an aliquot of each grain size. To investigate the effects of microstructure, in particular fission track density, separate aliquots were heated to temperatures of 200°C, 300°C, 400°C, 600°C, and 800°C for six hours after which they were cooled to room temperature and radon emanation rates were measured. Fission track densities were measured after the same annealing steps in the Mud Tank zircon, allowing quantification of 222Rn emanation rate as a function of fission track density. In general, radon emanation rates decrease with decreasing fission track density, but increase when all fission tracks are annealed, suggesting the possibility of using 222Rn to assess defect density within crystals. To investigate diffusive loss of 222Rn, we heated separate aliquots of each grain size of the Bancroft zircon to 975°C for different durations. 222Rn loss after heating was assessed by measuring the activity of the daughter products of 222Rn (214Bi and 214Pb), in addition to 226Ra, 228Ra, 234Th, and 210Pb, using gamma spectroscopy before and after heating. Results indicate slow diffusion of 222Rn, and suggest there may be structural changes in the zircon lattice at long heating durations. Results of both experiments have implications for U/Th-Pb geochronology (i.e., discordant ages), and noble gas escape systematics in zircon (i.e., volume diffusion or fast pathway escape).
机译:岩石和矿物产生的Rad是普遍存在的,但是of损失的机理尚不清楚。定量锆石中ra的散发率可能对锆石中U-Pb年龄的可靠性有潜在影响。 238U衰变链包括222Rn稀有气体,其半衰期为3.82天,如果存在足够的路径,则可以从锆石的晶体结构中逸出;如果母体238U非常靠近晶体的外边缘,则可以通过反冲而逸出。 222Rn的丧失最终导致206Pb的缺乏,导致238U-206Pb,235U-207Pb和232Th-208Pb年龄之间出现不一致。为了评估影响锆石中ra损失的因素,我们进行了两个实验:一个集中于微观结构对室温222Rn散发的影响,另一个研究了高温扩散引起的222Rn损失。本研究从三个地点中的每个地点选择了大(约100克)单晶锆石样品:泥浆罐,马拉维和班克罗夫特。将锆石粉碎,并分别分离出五种粒度(500微米,250-500微米,125-250微米,63-125微米和<63微米)。测量每个晶粒尺寸的等分试样的室温ra散发率。为了研究微观结构的影响,特别是裂变径迹密度,将单独的等分试样分别加热至200°C,300°C,400°C,600°C和800°C的温度达六个小时,然后冷却至室温测量温度和ra散发率。在Mud Tank锆石中进行相同的退火步骤后,测量了裂变径迹密度,从而可以根据裂变径迹密度对222Rn释放速率进行量化。通常,ra的散发率随裂变径迹密度的降低而降低,但当所有裂变径迹退火时都增加,这提示使用222Rn评估晶体中缺陷密度的可能性。为了研究222Rn的扩散损失,我们将Bancroft锆石的每种晶粒的等分试样分别加热到975°C,持续时间不同。通过测量加热前后的226Rn子产物(214Bi和214Pb)除226Ra,228Ra,234Th和210Pb之外的222Rn子产物的活性来评估加热后222Rn的损失。结果表明222Rn缓慢扩散,并表明在长时间加热下锆石晶格中可能存在结构变化。这两个实验的结果都对U / Th-Pb年代学(即年龄不一致)和锆石中稀有气体逸出系统(即体积扩散或快速通道逸出)有影响。

著录项

  • 作者

    Eakin, Marty.;

  • 作者单位

    Wayne State University.;

  • 授予单位 Wayne State University.;
  • 学科 Geology.
  • 学位 M.S.
  • 年度 2014
  • 页码 78 p.
  • 总页数 78
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

  • 入库时间 2022-08-17 11:53:17

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