Correction to “Experimental study on synchrotron radiation photoionization of secondary organic aerosol derived from styrene ozonolysis”

IF 16.4 1区 化学 Q1 CHEMISTRY, MULTIDISCIPLINARY Accounts of Chemical Research Pub Date : 2024-07-28 DOI:10.1002/jccs.202401004
{"title":"Correction to “Experimental study on synchrotron radiation photoionization of secondary organic aerosol derived from styrene ozonolysis”","authors":"","doi":"10.1002/jccs.202401004","DOIUrl":null,"url":null,"abstract":"<p>\n <span>M. -Q. Huang</span>, <span>H. -H. Wang</span>, <span>X. -B. Shan</span>, <span>L.-S. Sheng</span>, <span>C.-J. Hu</span>, <span>X. -J. Gu</span>, <span>W. -J. Zhang</span>\n </p><p><i>J. Chin. Chem. Soc</i>. <b>2023</b>, <i>70</i>, 938</p><p>https://doi.org/10.1002/jccs.202200557</p><p>In fact, photoionization mass spectra of styrene particles are obtained at under synchrotron radiation of 15.0, 12.5, and 10.0 eV. Due to our carelessness, the synchrotron radiation energy was mistakenly written as 15.0, 12.5, and 10.5 eV.</p><p>In this correction, we present the photoionization mass spectra of styrene particles with synchrotron radiation photon energies of 10.0, 12.5, and 15.0 eV, respectively. Meanwhile, the photon energy of synchrotron radiation in the text is modified. The main conclusions of the original work remain unaffected by the corrections. The corrections are as follows.</p><p>The VUV-PIMS in U14-A of the Hefei National Synchrotron Radiation Laboratory is used to detect styrene particles in real-time.</p><p><i>is replaced with</i></p><p>The synchrotron photon energy provided by U14-A is ranged from 8 to 16 eV. While photon energy at 10.5 eV is generally used to measure the photoionization mass spectrum of organic compounds in our previous studies.</p><p><i>is replaced with</i></p><p>photon energies of 10.5, 13.0, and 15.5 eV are selected successively in an increment of 2.5 eV for the measurement of styrene particles.</p><p><i>is replaced with</i></p><p>During the detection, the energy of the synchrotron radiation photon is 10.5 eV.</p><p><i>is replaced with</i></p><p>Figure 3 shows the photoionization mass spectra of styrene particles with synchrotron radiation photon energies of 10.5, 13.0, and 15.5 eV, respectively. The molecular ion (C<sub>8</sub>H<sub>8</sub><sup>+</sup>, m/z = 104) and protonated molecular ion peak (C<sub>8</sub>H<sub>9</sub><sup>+</sup>, m/z = 105) of styrene are detected when the photon energy is 10.5 eV.</p><p><i>is replaced with</i></p><p>When the photon energy is 13.0 eV, fragment peaks with m/z = 103 and m/z = 77 are detected. When the photon energy is 15.5 eV, the intensity of the peaks with m/z = 103 and m/z = 77 increases significantly. According to the structure of the styrene molecule, the peaks of m/z = 103 and m/z = 77 may be the fragmentation peaks generated by photodissociation of the hydrogen atom and vinyl group from the molecular ion peak.</p><p><i>is replaced with</i></p><p>However, photoionization efficiency curve (PIE) of styrene molecular ion (C<sub>8</sub>H<sub>8</sub><sup>+</sup>) shown in Figure 4 is the same as the PIE figure obtained by Kobayashi et al.(Kobayashi T., Phys. Lett. A 1978, 69, 105.)</p><p>Figure 4 displays the photoionization efficiency curve of the styrene molecular ion (C<sub>8</sub>H<sub>8</sub><sup>+</sup>). There is an obvious threshold at 8.46 eV, and the ionization potential of the styrene molecule (IP(C<sub>8</sub>H<sub>8</sub><sup>+</sup>)) is (8.46 ± 0.03) eV.</p><p><i>is replaced with</i></p><p>Also, the error bar is drawn with the average value as the midpoint and the standard deviation of the three repeated measurements as half of the line segment length, as shown in Figure 5.</p><p><i>is replaced with</i></p><p>Figure 5 The average corrected mass concentration of</p><p><i>is replaced with</i></p><p>Figure 6 Size distribution of stabilized styrene SOA particles</p><p><i>is replaced with</i></p><p>Figure 7 Photoionization mass spectra of styrene SOA particles at 10.5 eV photon energy.</p><p><i>is replaced with</i></p><p>Figure 6. The size of SOA particles formed from styrene.</p><p><i>is replaced with</i></p><p>Figure 7 is the photoionization mass spectra of styrene SOA particles measured at the photon energy of synchrotron radiation of 10.5 eV.</p><p><i>is replaced with</i></p><p>While the obtained photoionization efficiency curves in the range of 7.5–11.5 eV for m/z = 78, 94, 106, and 122 are shown in Figure 8.</p><p><i>is replaced with</i></p><p>As shown in Figure 8 and Table 1,</p><p><i>is replaced with</i></p><p>Figure 8 The photoionization efficiency curves</p><p><i>is replaced with</i></p><p>As shown in Figure 9</p><p><i>is replaced with</i></p><p>as illustrated in Figure 9</p><p><i>is replaced with</i></p><p>Figure 9 The suggested mechanism of ozone reaction with styrene to produce carbonyl and phenolic compounds.</p><p><i>is replaced with</i></p><p>as shown in Figure 7.</p><p><i>is replaced with</i></p><p>As shown in Figure 10</p><p><i>is replaced with</i></p><p>Figure 10 The UV–Vis spectra of extraction solution for</p><p><i>is replaced with</i></p><p>Figure 11 The infrared spectra of extraction solution for</p><p><i>is replaced with</i></p><p>Figure 11 is relatively strong</p><p><i>is replaced with</i></p><p>In the originally published version of the article, the importance of styrene is described in Introduction Section (Left column Line 2–6, Right column Line 1–7 on page 938, Left column Line 1–9 on page 939):</p><p>Styrene is an organic compound formed from substituting one hydrogen atom of benzene with vinyl group. As vinyl double bond can be polymerized, styrene as one of the most important monomers is widely used in the production of polystyrene, styrene butadiene rubber, styrene butadiene latex, and so forth [1, 2]. Styrene is discharged into atmosphere via natural sources such as plants and microorganisms, and solvent use, fuel combustion, industrial processes, and other anthropogenic sources [3–5]. Similar to other aromatic hydrocarbons, styrene is a harmful environmental pollutant in atmosphere. It is inherently toxic and can damage the central nervous and reproductive systems of the human body. It is also classified as a potential carcinogen by the International Cancer Research Institute of World Health Organization [6, 7]. In addition, styrene mainly undergoes reaction with ozone and other oxidant in atmosphere to form secondary organic aerosol (SOA) [8–12]. SOA particles can absorb and scatter sunlight, reduce atmospheric visibility [13, 14]. penetrate deep into the lungs and bronchus, and endanger human health [15].</p><p>However, there are some ambiguous sentences in these descriptions. In this correction, we revise these sentences. The main conclusions of the original work remain unaffected by the corrections. The corrections are as follows.</p><p>Styrene is the substance generated from substituting benzene's hydrogen atom by vinyl group. As vinyl double bond can be polymerized, styrene as the vital monomer is extensively utilized while manufacturing styrene butadiene rubber, polystyrene, and so forth [1, 2]. Apart from natural sources of microorganisms, plants, etc., industrial processes, fuel combustion, and other anthropogenic sources also discharge styrene into atmosphere [3–5]. Like other aromatics, styrene is a harmful environmental pollutant. It is inherently toxic and can vandalize the reproductive and central nervous systems of the human body. It is also classified as a potential carcinogen by the International Cancer Research Institute of World Health Organization [6, 7]. In addition, styrene mainly reacts with ozone and other oxidant in atmosphere to form secondary organic aerosol (SOA) [8–12]. SOA can scatter and absorb sunlight, reduce visibility [13, 14], and penetrate deep into the lungs and bronchus, endangering human health [15].</p>","PeriodicalId":1,"journal":{"name":"Accounts of Chemical Research","volume":null,"pages":null},"PeriodicalIF":16.4000,"publicationDate":"2024-07-28","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://onlinelibrary.wiley.com/doi/epdf/10.1002/jccs.202401004","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Accounts of Chemical Research","FirstCategoryId":"92","ListUrlMain":"https://onlinelibrary.wiley.com/doi/10.1002/jccs.202401004","RegionNum":1,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"CHEMISTRY, MULTIDISCIPLINARY","Score":null,"Total":0}
引用次数: 0

Abstract

M. -Q. Huang, H. -H. Wang, X. -B. Shan, L.-S. Sheng, C.-J. Hu, X. -J. Gu, W. -J. Zhang

J. Chin. Chem. Soc. 2023, 70, 938

https://doi.org/10.1002/jccs.202200557

In fact, photoionization mass spectra of styrene particles are obtained at under synchrotron radiation of 15.0, 12.5, and 10.0 eV. Due to our carelessness, the synchrotron radiation energy was mistakenly written as 15.0, 12.5, and 10.5 eV.

In this correction, we present the photoionization mass spectra of styrene particles with synchrotron radiation photon energies of 10.0, 12.5, and 15.0 eV, respectively. Meanwhile, the photon energy of synchrotron radiation in the text is modified. The main conclusions of the original work remain unaffected by the corrections. The corrections are as follows.

The VUV-PIMS in U14-A of the Hefei National Synchrotron Radiation Laboratory is used to detect styrene particles in real-time.

is replaced with

The synchrotron photon energy provided by U14-A is ranged from 8 to 16 eV. While photon energy at 10.5 eV is generally used to measure the photoionization mass spectrum of organic compounds in our previous studies.

is replaced with

photon energies of 10.5, 13.0, and 15.5 eV are selected successively in an increment of 2.5 eV for the measurement of styrene particles.

is replaced with

During the detection, the energy of the synchrotron radiation photon is 10.5 eV.

is replaced with

Figure 3 shows the photoionization mass spectra of styrene particles with synchrotron radiation photon energies of 10.5, 13.0, and 15.5 eV, respectively. The molecular ion (C8H8+, m/z = 104) and protonated molecular ion peak (C8H9+, m/z = 105) of styrene are detected when the photon energy is 10.5 eV.

is replaced with

When the photon energy is 13.0 eV, fragment peaks with m/z = 103 and m/z = 77 are detected. When the photon energy is 15.5 eV, the intensity of the peaks with m/z = 103 and m/z = 77 increases significantly. According to the structure of the styrene molecule, the peaks of m/z = 103 and m/z = 77 may be the fragmentation peaks generated by photodissociation of the hydrogen atom and vinyl group from the molecular ion peak.

is replaced with

However, photoionization efficiency curve (PIE) of styrene molecular ion (C8H8+) shown in Figure 4 is the same as the PIE figure obtained by Kobayashi et al.(Kobayashi T., Phys. Lett. A 1978, 69, 105.)

Figure 4 displays the photoionization efficiency curve of the styrene molecular ion (C8H8+). There is an obvious threshold at 8.46 eV, and the ionization potential of the styrene molecule (IP(C8H8+)) is (8.46 ± 0.03) eV.

is replaced with

Also, the error bar is drawn with the average value as the midpoint and the standard deviation of the three repeated measurements as half of the line segment length, as shown in Figure 5.

is replaced with

Figure 5 The average corrected mass concentration of

is replaced with

Figure 6 Size distribution of stabilized styrene SOA particles

is replaced with

Figure 7 Photoionization mass spectra of styrene SOA particles at 10.5 eV photon energy.

is replaced with

Figure 6. The size of SOA particles formed from styrene.

is replaced with

Figure 7 is the photoionization mass spectra of styrene SOA particles measured at the photon energy of synchrotron radiation of 10.5 eV.

is replaced with

While the obtained photoionization efficiency curves in the range of 7.5–11.5 eV for m/z = 78, 94, 106, and 122 are shown in Figure 8.

is replaced with

As shown in Figure 8 and Table 1,

is replaced with

Figure 8 The photoionization efficiency curves

is replaced with

As shown in Figure 9

is replaced with

as illustrated in Figure 9

is replaced with

Figure 9 The suggested mechanism of ozone reaction with styrene to produce carbonyl and phenolic compounds.

is replaced with

as shown in Figure 7.

is replaced with

As shown in Figure 10

is replaced with

Figure 10 The UV–Vis spectra of extraction solution for

is replaced with

Figure 11 The infrared spectra of extraction solution for

is replaced with

Figure 11 is relatively strong

is replaced with

In the originally published version of the article, the importance of styrene is described in Introduction Section (Left column Line 2–6, Right column Line 1–7 on page 938, Left column Line 1–9 on page 939):

Styrene is an organic compound formed from substituting one hydrogen atom of benzene with vinyl group. As vinyl double bond can be polymerized, styrene as one of the most important monomers is widely used in the production of polystyrene, styrene butadiene rubber, styrene butadiene latex, and so forth [1, 2]. Styrene is discharged into atmosphere via natural sources such as plants and microorganisms, and solvent use, fuel combustion, industrial processes, and other anthropogenic sources [3–5]. Similar to other aromatic hydrocarbons, styrene is a harmful environmental pollutant in atmosphere. It is inherently toxic and can damage the central nervous and reproductive systems of the human body. It is also classified as a potential carcinogen by the International Cancer Research Institute of World Health Organization [6, 7]. In addition, styrene mainly undergoes reaction with ozone and other oxidant in atmosphere to form secondary organic aerosol (SOA) [8–12]. SOA particles can absorb and scatter sunlight, reduce atmospheric visibility [13, 14]. penetrate deep into the lungs and bronchus, and endanger human health [15].

However, there are some ambiguous sentences in these descriptions. In this correction, we revise these sentences. The main conclusions of the original work remain unaffected by the corrections. The corrections are as follows.

Styrene is the substance generated from substituting benzene's hydrogen atom by vinyl group. As vinyl double bond can be polymerized, styrene as the vital monomer is extensively utilized while manufacturing styrene butadiene rubber, polystyrene, and so forth [1, 2]. Apart from natural sources of microorganisms, plants, etc., industrial processes, fuel combustion, and other anthropogenic sources also discharge styrene into atmosphere [3–5]. Like other aromatics, styrene is a harmful environmental pollutant. It is inherently toxic and can vandalize the reproductive and central nervous systems of the human body. It is also classified as a potential carcinogen by the International Cancer Research Institute of World Health Organization [6, 7]. In addition, styrene mainly reacts with ozone and other oxidant in atmosphere to form secondary organic aerosol (SOA) [8–12]. SOA can scatter and absorb sunlight, reduce visibility [13, 14], and penetrate deep into the lungs and bronchus, endangering human health [15].

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对 "苯乙烯臭氧分解产生的二次有机气溶胶同步辐射光离子化实验研究 "的更正
修改-删除了第 942 页的图 4在文章最初发表的版本中,图 4 显示了苯乙烯分子离子(C8H8+)的光电离效率曲线。然而,图 4 所示苯乙烯分子离子 (C8H8+) 的光电离效率曲线 (PIE) 与 Kobayashi 等人获得的 PIE 图相同(Kobayashi T., Phys. Lett. A 1978, 69, 105.)原文的主要结论不受更正影响。更正如下:删除第 942 页的图 4。修改--第 941 页中数字的编号(右栏从下往上第 21 行) 图 4 显示了苯乙烯分子离子(C8H8+)的光离子化效率曲线。苯乙烯分子离子 (C8H8+) 的光电离效率曲线在 8.46 eV 处有一个明显的阈值,苯乙烯分子 (IP(C8H8+)) 的电离势为 (8.46 ± 0.03) eV。修改--第 942 页中数字的编号(右栏第 9 行,从下往上排)另外,如图 5 所示,误差条的绘制以平均值为中点,三次重复测量的标准偏差为线段长度的一半。修改第 9437.1 页中的数字编号。 左栏第 1 行:图 5 平均修正质量浓度改为图 4 平均修正质量浓度为 7.2。 左栏第 6 行:图 6 稳定苯乙烯 SOA 粒子的尺寸分布改为图 5 稳定苯乙烯 SOA 粒子的尺寸分布 7.3。 右栏第 1 行:图 7 苯乙烯 SOA 粒子在 10.5 eV 光子能量下的光离子化质谱,替换为图 6 苯乙烯 SOA 粒子在 10.0 eV 光子能量下的光离子化质谱。7.4. 右栏第 3 行:图 6。用图 5 代替。苯乙烯形成的 SOA 粒子的尺寸。7.5. 右栏第 9 行:图 7 是在同步辐射光子能量为 10.5 eV 时测量的苯乙烯 SOA 粒子的光离子化质谱,替换为图 6 是在同步辐射光子能量为 10.0 eV 时测量的苯乙烯 SOA 粒子的光离子化质谱。7.6. 右栏第 19 行:图 8 显示了 m/z=78、94、106 和 122 在 7.5-11.5 eV 范围内的光电离效率曲线,将其替换为图 7 显示了 m/z=78、94、106 和 122 在 7.5-11.5 eV 范围内的光电离效率曲线。7.7. 右栏第 27 行:如图 8 和表 1 所示,改为如图 7 和表 1 所示,修改第 9448.1 页中的数字编号。 第 1 行:图 8 光离子化效率曲线改为图 7 光离子化效率曲线 8.2. 左栏 倒数第 2 行:如图 9 所示改为如图 8 所示 8.3. 右栏 倒数第 1 行:如图 9 所示改为如图 8 所示 修改第 9459.1 页中的数字编号。 第 1 行图 9 臭氧与苯乙烯反应生成羰基和酚类化合物的机理改为图 8 臭氧与苯乙烯反应生成羰基和酚类化合物的机理。9.2. 右栏自下而上第 7 行:如图 7 所示,替换为如图 6 所示。9.3. 右栏底部第 2 行:如图 10 所示改为如图 9 所示 修改第 94610.1 页中的数字编号。 左栏第 1 行:图 10 萃取液的紫外可见光谱替换为图 9 萃取液的紫外可见光谱 10.2. 左栏第 3 行:图 11 萃取液的红外光谱替换为图 10 10.3 萃取液的红外光谱。 第 938-939 页描述了苯乙烯的重要性在文章最初出版的版本中,"引言 "部分(第 938 页左栏第 2-6 行,右栏第 1-7 行,第 939 页左栏第 1-9 行)描述了苯乙烯的重要性:苯乙烯是用乙烯基取代苯的一个氢原子而形成的有机化合物。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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Accounts of Chemical Research
Accounts of Chemical Research 化学-化学综合
CiteScore
31.40
自引率
1.10%
发文量
312
审稿时长
2 months
期刊介绍: Accounts of Chemical Research presents short, concise and critical articles offering easy-to-read overviews of basic research and applications in all areas of chemistry and biochemistry. These short reviews focus on research from the author’s own laboratory and are designed to teach the reader about a research project. In addition, Accounts of Chemical Research publishes commentaries that give an informed opinion on a current research problem. Special Issues online are devoted to a single topic of unusual activity and significance. Accounts of Chemical Research replaces the traditional article abstract with an article "Conspectus." These entries synopsize the research affording the reader a closer look at the content and significance of an article. Through this provision of a more detailed description of the article contents, the Conspectus enhances the article's discoverability by search engines and the exposure for the research.
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