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高分辨率交叉束散射实验中速度映射离子图像的分析:教程综述。

Analysis of velocity-mapped ion images from high-resolution crossed-beam scattering experiments: a tutorial review.

作者信息

Zastrow Alexander von, Onvlee Jolijn, Parker David H, van de Meerakker Sebastiaan Y T

机构信息

Radboud University, Institute for Molecules and Materials, Heijendaalseweg 135, Nijmegen, 6525 AJ Netherlands.

出版信息

EPJ Tech Instrum. 2015;2(1):11. doi: 10.1140/epjti/s40485-015-0020-z. Epub 2015 Jul 28.

DOI:10.1140/epjti/s40485-015-0020-z
PMID:26322265
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC4551116/
Abstract

A Stark decelerator produces beams of molecules with high quantum state purity, and small spatial, temporal and velocity spreads. These tamed molecular beams are ideally suited for high-resolution crossed beam scattering experiments. When velocity map imaging is used, the Stark decelerator allows the measurement of scattering images with unprecedented radial sharpness and angular resolution. Differential cross sections must be extracted from these high-resolution images with extreme care, however. Common image analysis techniques that are used throughout in crossed beam experiments can result in systematic errors, in particular in the determination of collision energy, and the allocation of scattering angles to observed peaks in the angular scattering distribution. Using a high-resolution data set on inelastic collisions of velocity-controlled NO radicals with Ne atoms, we describe the challenges met by the high resolution, and present methods to mitigate or overcome them. 34.50.-s; 37.10.Mn.

摘要

斯塔克减速器能产生具有高量子态纯度、且空间、时间和速度展宽都很小的分子束。这些经过“驯服”的分子束非常适合用于高分辨率的交叉束散射实验。当使用速度成像技术时,斯塔克减速器能够以前所未有的径向清晰度和角分辨率测量散射图像。然而,必须极其小心地从这些高分辨率图像中提取微分截面。在交叉束实验中普遍使用的常规图像分析技术可能会导致系统误差,尤其是在碰撞能量的确定以及将散射角分配给角散射分布中观测到的峰时。通过使用关于速度可控的一氧化氮自由基与氖原子非弹性碰撞的高分辨率数据集,我们描述了高分辨率所面临的挑战,并提出了减轻或克服这些挑战的方法。34.50.-s;37.10.Mn。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1a84/4551116/a9c2b06b9848/40485_2015_20_Fig12_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1a84/4551116/d454daadf39e/40485_2015_20_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1a84/4551116/8a31dc3bbe97/40485_2015_20_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1a84/4551116/203f5290e3bc/40485_2015_20_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1a84/4551116/7a4d09b68775/40485_2015_20_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1a84/4551116/b32a1b2803c8/40485_2015_20_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1a84/4551116/2bf5675d20f3/40485_2015_20_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1a84/4551116/b249dcaedffe/40485_2015_20_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1a84/4551116/acb829c96a98/40485_2015_20_Fig8_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1a84/4551116/4f9f47f5ffb7/40485_2015_20_Fig9_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1a84/4551116/e228c2ea059f/40485_2015_20_Fig10_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1a84/4551116/8143e03f8e05/40485_2015_20_Fig11_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1a84/4551116/a9c2b06b9848/40485_2015_20_Fig12_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1a84/4551116/d454daadf39e/40485_2015_20_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1a84/4551116/8a31dc3bbe97/40485_2015_20_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1a84/4551116/203f5290e3bc/40485_2015_20_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1a84/4551116/7a4d09b68775/40485_2015_20_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1a84/4551116/b32a1b2803c8/40485_2015_20_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1a84/4551116/2bf5675d20f3/40485_2015_20_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1a84/4551116/b249dcaedffe/40485_2015_20_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1a84/4551116/acb829c96a98/40485_2015_20_Fig8_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1a84/4551116/4f9f47f5ffb7/40485_2015_20_Fig9_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1a84/4551116/e228c2ea059f/40485_2015_20_Fig10_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1a84/4551116/8143e03f8e05/40485_2015_20_Fig11_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1a84/4551116/a9c2b06b9848/40485_2015_20_Fig12_HTML.jpg

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本文引用的文献

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Phys Rev Lett. 2014 Dec 31;113(26):263202. doi: 10.1103/PhysRevLett.113.263202. Epub 2014 Dec 30.
2
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Phys Chem Chem Phys. 2014 Aug 14;16(30):15768-79. doi: 10.1039/c4cp01519c.
3
State-resolved diffraction oscillations imaged for inelastic collisions of NO radicals with He, Ne and Ar.为 NO 自由基与 He、Ne 和 Ar 的非弹性碰撞成像的态分辨衍射振荡。
观点:高级粒子成像。
J Chem Phys. 2017 Jul 7;147(1):013601. doi: 10.1063/1.4983623.
Nat Chem. 2014 Mar;6(3):216-21. doi: 10.1038/nchem.1860. Epub 2014 Feb 9.
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Rotational alignment effects in NO(X) + Ar inelastic collisions: an experimental study.NO(X) + Ar 非弹性碰撞中的旋转对准效应:一项实验研究。
J Chem Phys. 2013 Mar 14;138(10):104310. doi: 10.1063/1.4792159.
5
Rotational alignment effects in NO(X) + Ar inelastic collisions: a theoretical study.NO(X) + Ar 非弹性碰撞中的旋转对准效应:理论研究。
J Chem Phys. 2013 Mar 14;138(10):104309. doi: 10.1063/1.4792158.
6
A new high intensity and short-pulse molecular beam valve.一种新型的高强度短脉冲分子束阀。
Rev Sci Instrum. 2013 Feb;84(2):023102. doi: 10.1063/1.4790176.
7
Ab initio ground- and excited-state intermolecular potential energy surfaces for the NO-Ne and NO-Ar van der Waals complexes.从头算基态和激发态 NO-Ne 和 NO-Ar 范德华复合物的分子间势能面。
J Phys Chem A. 2012 Jul 12;116(27):7319-28. doi: 10.1021/jp303573a. Epub 2012 Jun 29.
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Manipulation and control of molecular beams.分子束的操控与控制。
Chem Rev. 2012 Sep 12;112(9):4828-78. doi: 10.1021/cr200349r. Epub 2012 Mar 27.
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Fully Λ-doublet resolved state-to-state differential cross-sections for the inelastic scattering of NO(X) with Ar.完全 Λ-双重态分辨态态态分辨态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态态 态态态态态态态态态态态态态态态 状态至状态 的微分截面 解析: 这段英文文本是关于化学领域的内容,涉及分子反应动力学的研究。这段话中,"differential cross-section"表示微分截面,是指在量子力学中描述微观粒子散射或碰撞过程中,粒子散射角不同时的散射几率的一种物理量;"inelastic scattering"表示非弹性散射,是指微观粒子和物质原子之间发生非弹性碰撞时的散射过程;"NO(X)"指一氧化氮分子;"Ar"指氩气;"inelastic scattering of Ar with NO(X)"则表示氩气与一氧化氮分子之间的非弹性散射过程。
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Phys Chem Chem Phys. 2010 Sep 28;12(36):10660-70. doi: 10.1039/c004422a. Epub 2010 Jul 23.