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Diamondoids Under Pressure 压力下的金刚石
Pub Date : 2020-03-24 DOI: 10.1002/9781119508229.ch27
Sulgiye Park, Yu Lin, W. Mao
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引用次数: 0
Crystallization of Water Mediated by Carbon 碳介导的水结晶
Pub Date : 2020-03-24 DOI: 10.1002/9781119508229.ch8
Tianshu Li, Yuanfei Bi, Boxiao Cao
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引用次数: 0
The Changing Character of Carbon in Fluids with Pressure 流体中碳随压力的变化特性
Pub Date : 2020-03-24 DOI: 10.1002/9781119508229.ch22
D. Sverjensky, I. Daniel, A. V. Brovarone
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引用次数: 13
Nitrogen Diffusion in Calcite 方解石中的氮扩散
Pub Date : 2020-03-24 DOI: 10.1002/9781119508229.ch10
D. Cherniak, M. Schaller, B. Watson
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引用次数: 0
The Optimization of Zircon Analyses by Laser‐Assisted Atom Probe Microscopy 激光辅助原子探针显微法分析锆石的优化
Pub Date : 2017-12-01 DOI: 10.1002/9781119227250.CH14
D. Saxey, S. Reddy, D. Fougerouse, W. Rickard
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引用次数: 17
Best Practices for Reporting Atom Probe Analysis of Geological Materials 报告地质材料原子探针分析的最佳实践
Pub Date : 2017-12-01 DOI: 10.1002/9781119227250.CH18
T. Blum, J. Darling, T. Kelly, D. Larson, D. Moser, A. Pérez-Huerta, T. Prosa, S. Reddy, D. Reinhard, D. Saxey, R. Ulfig, J. Valley
Recent work has established atom probe tomography (APT) as a unique tool within the geosciences for interrogat­ ing material chemistry at the nanoscale. In APT, a needle‐ shaped specimen with an end‐form radius on the order of 50–100 nm is held at high voltage, and constituent atoms are field evaporated through application of a timed voltage pulse (for conductive materials) or laser pulse (for semicon­ ductors and insulators). The voltage bias and small radius of curvature produce a large electric field that is localized around, and diverging from, the end surface of the needle‐ shaped specimen; evaporated ions are accelerated by the local electric field, leading to divergent trajectories for ions originating from different positions on the specimen surface. A position‐sensitive detector records both the hit position of Best Practices for Reporting Atom Probe Analysis of Geological Materials
最近的工作已经建立了原子探针断层扫描(APT)作为一个独特的工具,在地球科学审问材料化学在纳米尺度。在APT中,将端形半径为50 - 100nm的针状试样置于高压下,并通过施加定时电压脉冲(用于导电材料)或激光脉冲(用于半导体和绝缘体)将其组成原子进行场蒸发。电压偏置和小曲率半径产生了一个大的电场,该电场位于针状试样的端面周围,并从端面发散出来;蒸发的离子被局部电场加速,导致来自试样表面不同位置的离子产生不同的轨迹。位置敏感探测器记录了报告地质材料原子探针分析的最佳实践的击中位置
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引用次数: 28
Detecting Micro‐ and Nanoscale Variations in Element Mobility in High‐Grade Metamorphic Rocks 高品位变质岩中元素迁移率的微纳米尺度变化研究
Pub Date : 2017-12-01 DOI: 10.1002/9781119227250.CH13
M. Kusiak, S. Wilde, R. Wirth, M. Whitehouse, D. Dunkley, I. Lyon, S. Reddy, A. Berry, M. D. Jonge
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引用次数: 7
Dawn-dusk asymmetries in the auroral particle precipitation and their modulations by substorms 极光粒子降水的黎明-黄昏不对称性及其受亚暴的调制
Pub Date : 2017-10-20 DOI: 10.1002/9781119216346.CH20
S. Wing, J. Johnson, E. Camporeale
textabstractAuroral particle precipitation exhibits dawn-dusk asymmetries that reflect the asymmetries in the particle populations, waves, and processes in the magnetosphere. The diffuse auroral electrons can be observed mainly in 22:00 – 09:00 MLT, which coincides much with the spatial distribution of the whistler-mode chorus waves that have been shown to be the predominant mechanism for pitch-angle scatterring magnetospheric electrons into the loss cone. On the other hand, the monoenergetic auroral electrons can be observed at dusk-midnight sector. The monoenergetic electrons are magnetospheric electrons that have gone through a quasi-static parallel electric field in the upward field-aligned current regions. The broadband auroral electrons can be found mostly at 22:00 – 02:00 MLT where a peak in the Poynting flux of Alfven waves is observed. Alfven waves are known to cause broadband acceleration of electrons. There may be a connection between monoenergetic and broadband electrons in that the low frequency Alfven wave–electron interaction can result in monoenergetic electron signature. Substorms increase the power of the diffuse, monoenergetic, and broadband electron aurora by 310%, 71%, and 170%, respectively. The duration of the substorm cycle for monenergetic and broadband auroral is ~5 hr, but it is larger than 5 hr for diffuse auroral electrons.
大气粒子降水呈现出黎明-黄昏的不对称性,这反映了磁层中粒子数量、波和过程的不对称性。弥漫性极光电子主要出现在22点~ 9点,这与哨声模式合唱波的空间分布非常吻合,哨声模式合唱波是俯角散射磁层电子进入损耗锥的主要机制。另一方面,单能量的极光电子可以在黄昏-午夜扇区被观察到。单能电子是磁层电子,它们在向上场对准的电流区域中经历了准静态平行电场。宽频带极光电子主要出现在22:00 - 02:00 MLT,在此期间阿尔芬波的波印亭通量出现峰值。众所周知,阿尔芬波会引起电子的宽带加速。单能电子与宽带电子之间可能存在联系,低频阿尔芬波与电子相互作用可导致单能电子的特征。亚暴使漫射、单能和宽带电子极光的能量分别增加310%、71%和170%。单能和宽带极光的亚暴周期持续时间约为5小时,而漫射极光电子的亚暴周期持续时间大于5小时。
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引用次数: 2
Mechanisms Explaining Recent Changes in Australian Climate Extremes 解释最近澳大利亚极端气候变化的机制
Pub Date : 2017-06-19 DOI: 10.1002/9781119068020.CH15
S. Lewis, D. Karoly, A. King, S. Perkins, M. Donat
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引用次数: 5
Timing of Anthropogenic Emergence in Climate Extremes 极端气候中人为出现的时间
Pub Date : 2017-06-19 DOI: 10.1002/9781119068020.CH6
A. King, M. Donat, E. Hawkins, D. Karoly
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引用次数: 4
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Geophysical monograph
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