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2
Conversion of He(2 S) to He( aΣ ) in Liquid Helium.液氦中He(2 S) 向He( aΣ ) 的转换
J Phys Chem Lett. 2018 Oct 18;9(20):6017-6023. doi: 10.1021/acs.jpclett.8b02454. Epub 2018 Oct 4.
3
Vibrational Spectroscopy of Fluoroformate, FCO, Trapped in Helium Nanodroplets.捕获于氦纳米液滴中的氟甲酸酯(FCO)的振动光谱
J Phys Chem Lett. 2018 May 3;9(9):2305-2310. doi: 10.1021/acs.jpclett.8b00664. Epub 2018 Apr 23.
4
Microsolvation of phthalocyanine molecules in superfluid helium nanodroplets as revealed by the optical line shape at electronic origin.酞菁分子在超流氦纳米液滴中的微溶剂化作用,如电子起源处的光学线形状所揭示的那样。
J Chem Phys. 2018 Apr 14;148(14):144301. doi: 10.1063/1.5022006.
5
Formation of He via electron impact of helium droplets.氦通过氦液滴的电子碰撞形成。
J Chem Phys. 2018 Jan 28;148(4):044302. doi: 10.1063/1.5001715.
6
Doping of Green Fluorescent Protein into Superfluid Helium Droplets: Size and Velocity of Doped Droplets.将绿色荧光蛋白掺杂到超流氦滴中:掺杂液滴的尺寸和速度。
J Phys Chem A. 2017 Sep 14;121(36):6671-6678. doi: 10.1021/acs.jpca.7b05718. Epub 2017 Aug 31.
7
Electron impact ionization and multiphoton ionization of doped superfluid helium droplets: A comparison.掺杂超流氦滴的电子碰撞电离和多光子电离:比较
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8
Synthesis of nanoparticles in helium droplets-A characterization comparing mass-spectra and electron microscopy data.氦滴中纳米颗粒的合成——质谱与电子显微镜数据对比的表征
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9
Facile time-of-flight methods for characterizing pulsed superfluid helium droplet beams.用于表征脉冲超流氦滴束的简便飞行时间方法。
Rev Sci Instrum. 2015 Aug;86(8):084102. doi: 10.1063/1.4928107.
10
Effect of kinetic energy on the doping efficiency of cesium cations into superfluid helium droplets.动能对铯阳离子掺杂到超流氦滴中的效率的影响。
J Chem Phys. 2015 Jul 28;143(4):044310. doi: 10.1063/1.4927471.

掺杂多价阳离子和大离子化氦液滴中电荷转移失败。

Doping with multiple cations and failure of charge transfer in large ionized helium droplets.

机构信息

Department of Chemistry, Oregon State University, Corvallis, Oregon 97331-4003, USA.

出版信息

J Chem Phys. 2019 Oct 7;151(13):134307. doi: 10.1063/1.5123735.

DOI:10.1063/1.5123735
PMID:31594345
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC7043853/
Abstract

We report experimental observations of aniline (A) cations and He when aniline is doped into ionized helium droplets. Large droplets containing 10 atoms are bombarded by energetic electrons, resulting in more than one positive charge in one droplet. When aniline encounters the charged droplets, some are ionized via charge transfer, while others can remain neutral in the presence of He when the mass-to-charge ratio (m/z) of the droplet is sufficiently large. Upon resonant excitation of the dopant A or A (n ≥ 1), He can be ejected. The excitation spectrum of He becomes a juxtaposition of the spectra of A and A . Moreover, an anticorrelation between the yields of He and A is observed with increasing energies of the ionizing electrons. We attribute this result to the combined effect of reduction in m/z of the droplets and the different locations of He and neutral A. Limited by the penetration depths of the ionizing electrons and further assisted by the Coulomb repulsion of coexisting cations, He is located within 20 nm of the surface, while neutral A has an average position inside a large droplet. Upon resonant excitation of the interior A, He is preferentially ejected. With increasing energies of the colliding electrons, the m/z of the droplets are reduced, leading to less effective charge shielding and more effective charge transfer, until ultimately, all He can be neutralized to form A.

摘要

我们报告了在苯胺掺杂到离子化氦液滴中时对苯胺(A)阳离子和 He 的实验观察结果。含有 10 个原子的大液滴被高能电子轰击,导致一个液滴中带有一个以上的正电荷。当苯胺遇到带电液滴时,一些通过电荷转移而被电离,而另一些在 m/z 足够大时,在存在 He 的情况下保持中性。当掺杂剂 A 或 A (n ≥ 1)被共振激发时,He 可以被逐出。He 的激发光谱成为 A 和 A 的光谱的并置。此外,随着离子化电子能量的增加,观察到 He 和 A 的产额之间存在反相关关系。我们将这一结果归因于液滴 m/z 的降低和 He 与中性 A 的不同位置的综合影响。受离子化电子的穿透深度的限制,并进一步受到共存阳离子的库仑排斥的辅助,He 位于表面 20nm 以内,而中性 A 位于大液滴内部。在内部 A 的共振激发下,He 被优先逐出。随着碰撞电子能量的增加,液滴的 m/z 降低,导致电荷屏蔽效果降低,电荷转移效果增强,直到最终,所有 He 都可以被中和形成 A。