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大气压下丁酰苯分子及碎片离子形成的高电场隧道电离量子化学分析

Quantum Chemical Analysis of the Molecular and Fragment Ion Formation of Butyrophenone by High-Electric Field Tunnel Ionization at Atmospheric Pressure.

作者信息

Takayama Mitsuo

机构信息

Graduate School of Nanobioscience, Yokohama City University, 22-2 Seto, Kanazawa-ku, Yokohama 236-0027, Japan.

出版信息

Mass Spectrom (Tokyo). 2024;13(1):A0156. doi: 10.5702/massspectrometry.A0156. Epub 2024 Oct 25.

DOI:10.5702/massspectrometry.A0156
PMID:39479219
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC11522704/
Abstract

The molecular ion M was observed when the liquid sample of butyrophenone was supplied using atmospheric pressure corona discharge (APCD). In contrast, the vapor supply resulted in the formation of the protonated molecule [M+H]. The mass spectrum obtained with the liquid supply showed two distinctive fragment ions at 105 and 120, resulting from α-cleavage and McLafferty rearrangement (McLR), respectively. The APCD spectrum showed peaks of M and the characteristic two fragment ions that were the same as the field ionization mass spectra of butyrophenone as reported by Chait . and Beckey . The formation of the molecular and fragment ions strongly indicated that high-electric field tunnel ionization (HEFTI) occurs by the HEF strength exceeding 10 V/m at the tip of the corona needle in APCD. The charge and spin density distributions of the molecular and fragment ions were analyzed by quantum chemical calculations using time-dependent density functional theory (TDDFT) and natural bond orbital (NBO) analysis.

摘要

当使用大气压电晕放电(APCD)提供丁酰苯的液体样品时,观察到了分子离子M。相比之下,蒸汽供应导致形成质子化分子[M+H]。液体供应获得的质谱显示在105和120处有两个独特的碎片离子,分别由α-裂解和麦克拉弗蒂重排(McLR)产生。APCD光谱显示了M的峰以及与Chait和Beckey报道的丁酰苯的场电离质谱相同的特征性两个碎片离子峰。分子离子和碎片离子的形成强烈表明,在APCD中,电晕针尖端的高电场强度超过10 V/m时会发生高电场隧道电离(HEFTI)。使用含时密度泛函理论(TDDFT)和自然键轨道(NBO)分析通过量子化学计算对分子离子和碎片离子的电荷和自旋密度分布进行了分析。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/70b4/11522704/10346ca48c4c/massspectrometry-13-1-A0156-figure10.jpg
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https://cdn.ncbi.nlm.nih.gov/pmc/blobs/70b4/11522704/10346ca48c4c/massspectrometry-13-1-A0156-figure10.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/70b4/11522704/20fa4aacf732/massspectrometry-13-1-A0156-figure09.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/70b4/11522704/42459b28b3ac/massspectrometry-13-1-A0156-figure01.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/70b4/11522704/896ad276979f/massspectrometry-13-1-A0156-figure02.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/70b4/11522704/2e5b2517dc13/massspectrometry-13-1-A0156-figure03.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/70b4/11522704/b149ba82f538/massspectrometry-13-1-A0156-figure04.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/70b4/11522704/3cdd262588ae/massspectrometry-13-1-A0156-figure05.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/70b4/11522704/38b4cc47b133/massspectrometry-13-1-A0156-figure06.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/70b4/11522704/d7e5f80f78bb/massspectrometry-13-1-A0156-figure07.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/70b4/11522704/d4d0a81f0b28/massspectrometry-13-1-A0156-figure08.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/70b4/11522704/10346ca48c4c/massspectrometry-13-1-A0156-figure10.jpg

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本文引用的文献

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The Surprising Dynamics of the McLafferty Rearrangement.麦克拉弗蒂重排的惊人动力学
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