Article(id=1320889305627738921, tenantId=1146029695717560320, journalId=1260987677001138203, issueId=1320888908896907909, articleNumber=null, orderNo=null, doi=10.13386/j.issn1002-0306.2025020096, pmid=null, cstr=null, oa=null, hot=null, price=null, onlineType=0, articleFormat=0, articleType=null, articleTypeStr=null, receivedDate=1739721600000, receivedDateStr=2025-02-17, revisedDate=null, revisedDateStr=null, acceptedDate=null, acceptedDateStr=null, onlineDate=1792854151398, onlineDateStr=2026-10-24, pubDate=1772294400000, pubDateStr=2026-03-01, doiRegisterDate=null, doiRegisterDateStr=null, onlineIssueDate=1792854151398, onlineIssueDateStr=2026-10-24, onlineJustAcceptDate=null, onlineJustAcceptDateStr=null, onlineFirstDate=null, onlineFirstDateStr=null, sourceXml=null, magXml=null, createTime=1792854151398, creator=13701087609, updateTime=1792854151398, updator=13701087609, issue=Issue{id=1320888908896907909, tenantId=1146029695717560320, journalId=1260987677001138203, year='2026', volume='47', issue='5', pageStart='1', pageEnd='503', issueExtLink='null', onlineDate='null', pubDate='1772294400000', pubDateStr='2026-03-01', beforeIssueId=null, nextIssueId=null, price=null, status=1, issueComplete=1, articleOrder=1, issueType=-1, specialIssue=null, createTime=1792854056809, creator='13701087609', updateTime=1792854056809, updator='13701087609', preIssue=null, nextIssue=null, articleTotal=null, ext=null, issueFiles=null, downloadFileDto=null}, startPage=92, endPage=100, ext={EN=ArticleExt(id=1320889305866814250, articleId=1320889305627738921, tenantId=1146029695717560320, journalId=1260987677001138203, language=EN, title=Mechanism of Photoisomerization of Astaxanthin: Experimental and Quantum Chemistry Study, columnId=1261336277291548795, journalTitle=Science and Technology of Food Industry, columnName=Research and Investigation, runingTitle=null, highlight=null, articleAbstract=

To investigate the photoisomerization mechanism of astaxanthin (AST), the types and contents of Z-configuration in photocatalytic conversion of AST were analyzed by HPLC and Q value method. Additionally, the AST configuration was optimized and frequency analysis was performed using density functional theory (DFT). Thermodynamic, kinetic, and energetic parameters of all-E- and Z-AST isomers were further calculated. The results demonstrated that 9-Z- and 13-Z-isomers were predominantly generated under photocatalysis, with the 13-Z content (17.72%) being significantly higher than 9-Z (13.57%) (P<0.05). Upon illumination, neutral AST molecules generated diradicals, facilitating bond twisting. All-E AST exhibited the smallest frontier orbital energy gap, promoting its transition from the ground state to the excited state, and subsequent isomerization into other configurations. Gibbs free energy analysis revealed the following stability order of AST isomers: all-E>9-Z>13-Z>15-Z, basically consistent with experimental observations. Moreover, the activation energy for all-E→9-Z conversion was higher than for all-E→15-Z/13-Z, while single-Z→double-Z isomerization required significantly higher energy than all-E→mono-Z conversion. Notably, the 13-Z-isomer formation rate was about 4-fold and 100-fold higher than that of 15-Z> and 9-Z, respectively. The negligible tunneling effect during mutual transformation explained the scarcity of multi-Z-isomers in experiments and the predominance of 13-Z over 9-Z AST. Collectively, these findings elucidate the controlled generation mechanism of AST isomers and establish a theoretical framework for carotenoid isomerization.

, authors=Lesong ZHOU, Xiaojun ZOU, Jialing CHEN, Jie XIAO, Yong CAO, Xiaojuan LIU*, authorsList=Lesong ZHOU, Xiaojun ZOU, Jialing CHEN, Jie XIAO, Yong CAO, Xiaojuan LIU, authorCompany=null, correspAuthors=Xiaojuan LIU, authorNote=null, correspAuthorsNote=null, copyrightStatement=Copyright © 2026 Science and Technology of Food Industry. All rights reserved., copyrightOwner=null, extLink=null, articleAbsUrl=null, sourceXml=null, magXml=null, pdfUrl=null, pdf=null, pdfFileSize=null, pdfExtLink=null, richHtmlUrl=null, mobilePdfUrl=null, reviewReport=null, pdfFirstPage=null, abstractGraph=null, abstractGraphContent=null, abstractVideo=null, citation=null, cebUrl=null, magXmlContent=null, mapNumber=null, fund=null), CN=ArticleExt(id=1320889309025125181, articleId=1320889305627738921, tenantId=1146029695717560320, journalId=1260987677001138203, language=CN, title=虾青素光异构化机理:实验与量子化学相结合研究, columnId=1261336277849391232, journalTitle=食品工业科技, columnName=研究与探讨, runingTitle=null, highlight=null, articleAbstract=

为探究虾青素(astaxanthin,AST)的光异构化机理,采用HPLC技术和Q值法分析光催化转化AST的顺式构型种类和含量,通过密度泛函理论对AST构型进行优化与频率分析,计算得到全反式(all-E)和顺式(Z)AST相互转化的热力学、动力学和能量参数。结果表明,全反式AST在光催化下主要形成9顺式(9-Z)和13顺式(13-Z),13-Z含量(17.72%)显著高于9-Z(13.57%)(P<0.05)。光照后,中性AST分子形成双自由基,双键容易发生扭转。全反式AST的前线轨道能隙差最小,更容易从基态转变为激发态,从而异构为其它构型;根据吉布斯自由能,AST异构体的相对稳定性顺序为:全反式>9-Z>13-Z>15-Z,与实验结果趋势基本相符;全反式AST形成9-Z的活化能高于15-Z和13-Z,单顺式AST转化为多顺式的活化能远高于全反式AST转化为单顺式异构体;13-Z构型生成速率分别约为15-Z和9-Z的4倍和100倍,且相互转化的隧穿效应可以忽略不计,与实验中多顺式异构体难以观察到相吻合,同时阐明实验中出现的13-Z AST比例显著高于9-Z的原因。研究结果揭示了AST可控实现异构体的生成机制,同时为其它类胡萝卜素异构化研究提供理论基础。

, authors=周乐松, 邹晓君, 陈佳玲, 肖杰, 曹庸, 刘晓娟*, authorsList=周乐松, 邹晓君, 陈佳玲, 肖杰, 曹庸, 刘晓娟, authorCompany=null, correspAuthors=刘晓娟, authorNote=

周乐松(1998−),男,硕士研究生,研究方向:功能食品学,食品生物化学及营养学,E-mail:

, correspAuthorsNote=
刘晓娟(1980−),女,博士,教授,研究方向:功能食品学、食品生物化学及营养学,E-mail:。
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周乐松(1998−),男,硕士研究生,研究方向:功能食品学,食品生物化学及营养学,E-mail:

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Journal of Agricultural and Food Chemistry, 2017, 65(4): 818−826., articleTitle=null, refAbstract=null)], funds=null, companyList=[AuthorCompany(id=1320889309226451774, tenantId=1146029695717560320, journalId=1260987677001138203, articleId=1320889305627738921, xref=null, ext=[AuthorCompanyExt(id=1320889309234840383, tenantId=1146029695717560320, journalId=1260987677001138203, articleId=1320889305627738921, companyId=1320889309226451774, language=EN, country=null, province=null, city=null, postcode=null, companyName=null, departmentName=null, remark=College of Food Science, South China Agricultural University, Guangdong Provincial Key Laboratory of Nutraceuticals and Functional Foods, Guangzhou 510642, China), AuthorCompanyExt(id=1320889309239034688, tenantId=1146029695717560320, journalId=1260987677001138203, articleId=1320889305627738921, companyId=1320889309226451774, language=CN, country=null, province=null, city=null, postcode=null, companyName=null, departmentName=null, remark=华南农业大学食品学院,广东省功能食品活性物重点实验室,广东广州 510642)])], figs=[ArticleFig(id=1320889311596233577, tenantId=1146029695717560320, journalId=1260987677001138203, articleId=1320889305627738921, language=EN, label=Fig.1, caption=HPLC chromatograms of AST after photoisomerization (A), all-E (B), 9-Z (C) and 13-Z (D) astaxanthin and corresponding electronic absorption spectra (E~G), figureFileSmall=Omm/PBga+oNkMq11FH7xDQ==, figureFileBig=bBrOsZKKMnFBWe/EC8wLbQ==, tableContent=null), ArticleFig(id=1320889311675925354, tenantId=1146029695717560320, journalId=1260987677001138203, articleId=1320889305627738921, language=CN, label=图1, caption=光异构化AST(A)、全反式(B)、9顺式(C)、13顺式(D)AST的HPLC色谱图以及对应的电子吸收光谱(E~G), figureFileSmall=Omm/PBga+oNkMq11FH7xDQ==, figureFileBig=bBrOsZKKMnFBWe/EC8wLbQ==, tableContent=null), ArticleFig(id=1320889311881446251, tenantId=1146029695717560320, journalId=1260987677001138203, articleId=1320889305627738921, language=EN, label=Fig.2, caption=Structure of neutral and di-radical forms of all-E (A), 9-Z (B), 13-Z (C) and 15-Z (D) astaxanthin, figureFileSmall=Jo/EKV8ktu5+aN9iEyVeRg==, figureFileBig=Gx+TuDOkWFdONNgyh9Ivdw==, tableContent=null), ArticleFig(id=1320889311948555116, tenantId=1146029695717560320, journalId=1260987677001138203, articleId=1320889305627738921, language=CN, label=图2, caption=全反式(A)、9顺式(B)、13顺式(C)和15顺式(D)AST中性和双自由基形式的结构, figureFileSmall=Jo/EKV8ktu5+aN9iEyVeRg==, figureFileBig=Gx+TuDOkWFdONNgyh9Ivdw==, tableContent=null), ArticleFig(id=1320889312015663981, tenantId=1146029695717560320, journalId=1260987677001138203, articleId=1320889305627738921, language=EN, label=Fig.3, caption=Molecular structure of all-E (A), 9-Z (B), 13-Z (C) and 15-Z (D) astaxanthin, figureFileSmall=porVXuMkTS+50/S6QFr5AQ==, figureFileBig=uROLzIWJM/3oNGAhblwqbw==, tableContent=null), ArticleFig(id=1320889312086967150, tenantId=1146029695717560320, journalId=1260987677001138203, articleId=1320889305627738921, language=CN, label=图3, caption=全反式(A)、9顺式(B)、13顺式(C)和15顺式(D)AST的分子结构, figureFileSmall=porVXuMkTS+50/S6QFr5AQ==, figureFileBig=uROLzIWJM/3oNGAhblwqbw==, tableContent=null), ArticleFig(id=1320889312149881711, tenantId=1146029695717560320, journalId=1260987677001138203, articleId=1320889305627738921, language=EN, label=Fig.4, caption=Specific bond length parameters of neutral and diatomic radicals of all-E (A), 9-Z (B), 13-Z (C) and 15-Z (D) astaxanthin, figureFileSmall=ks8JTJbh4r5rChkZyN9qFw==, figureFileBig=cH/S10qebYt20piYFs85tw==, tableContent=null), ArticleFig(id=1320889312225379184, tenantId=1146029695717560320, journalId=1260987677001138203, articleId=1320889305627738921, language=CN, label=图4, caption=全反式(A)、9顺式(B)、13顺式(C)和15顺式(D)AST的中性和双自由基两种形态特定键长参数

注:a:中性;b:双自由基;键长以Å表示和二面角参数ζ(单位为°)。

, figureFileSmall=ks8JTJbh4r5rChkZyN9qFw==, figureFileBig=cH/S10qebYt20piYFs85tw==, tableContent=null), ArticleFig(id=1320889312313459569, tenantId=1146029695717560320, journalId=1260987677001138203, articleId=1320889305627738921, language=EN, label=Fig.5, caption=Frontline molecular orbital energy diagrams of all-E (A), 9-Z (B), 13-Z (C) and 15-Z (D) astaxanthin, figureFileSmall=BbDE1c0YoZx0sNu9uzWzRg==, figureFileBig=xSOIoLrInLgIYbEE/F5Yzw==, tableContent=null), ArticleFig(id=1320889312384762738, tenantId=1146029695717560320, journalId=1260987677001138203, articleId=1320889305627738921, language=CN, label=图5, caption=全反式(A)、9顺式(B)、13顺式(C)和15顺式(D)AST的前线分子轨道能级图

注:红色表示正值部分,绿色表示负值部分,代表相位和相互之间的作用。HOMO最高占据轨道,LUMO最低未占轨道。

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Retention time, absorption wavelength and Q value of astaxanthin isomers

, figureFileSmall=null, figureFileBig=null, tableContent=
峰AST
异构体
保留
时间(min)
顺式峰
波长(nm)
主峰波长
(nm)
Q值
测定值报道值[8,20]
峰1全反式8.313734690.110.09−
峰29顺式11.343814770.150.110.20
峰313顺式12.273714670.550.550.52
), ArticleFig(id=1320889313076822908, tenantId=1146029695717560320, journalId=1260987677001138203, articleId=1320889305627738921, language=CN, label=表1, caption=

虾青素异构体保留时间、吸收波长及其Q值

, figureFileSmall=null, figureFileBig=null, tableContent=
峰AST
异构体
保留
时间(min)
顺式峰
波长(nm)
主峰波长
(nm)
Q值
测定值报道值[8,20]
峰1全反式8.313734690.110.09−
峰29顺式11.343814770.150.110.20
峰313顺式12.273714670.550.550.52
), ArticleFig(id=1320889313164903293, tenantId=1146029695717560320, journalId=1260987677001138203, articleId=1320889305627738921, language=EN, label=Table 2, caption=

Gibbs free energy difference obtained by single point energy correction of astaxanthin

, figureFileSmall=null, figureFileBig=null, tableContent=
AST构型/状态中性分子(kcal/mol)双自由基(kcal/mol)
全反式00
9顺式1.502.14
13顺式1.72−14.39
15顺式2.66−12.64
), ArticleFig(id=1320889313252983678, tenantId=1146029695717560320, journalId=1260987677001138203, articleId=1320889305627738921, language=CN, label=表2, caption=

虾青素单点能修正得到吉布斯自由能差

, figureFileSmall=null, figureFileBig=null, tableContent=
AST构型/状态中性分子(kcal/mol)双自由基(kcal/mol)
全反式00
9顺式1.502.14
13顺式1.72−14.39
15顺式2.66−12.64
), ArticleFig(id=1320889313324286847, tenantId=1146029695717560320, journalId=1260987677001138203, articleId=1320889305627738921, language=EN, label=Table 3, caption=

HOMO and LUMO energies and energy gaps of all-E, 9-Z, 13-Z and 15-Z neutral astaxanthin

, figureFileSmall=null, figureFileBig=null, tableContent=
中性ASTHOMO(au)LUMO(au)HOMO−LUMO(au)
全反式−0.10298−0.178920.07594
9顺式−0.10151−0.178750.07724
13顺式−0.10147−0.179720.07825
15顺式−0.10207−0.18020.07819
), ArticleFig(id=1320889313403978625, tenantId=1146029695717560320, journalId=1260987677001138203, articleId=1320889305627738921, language=CN, label=表3, caption=

全反式、9顺式、13顺式、15顺式中性AST的HOMO和LUMO能量及能隙

, figureFileSmall=null, figureFileBig=null, tableContent=
中性ASTHOMO(au)LUMO(au)HOMO−LUMO(au)
全反式−0.10298−0.178920.07594
9顺式−0.10151−0.178750.07724
13顺式−0.10147−0.179720.07825
15顺式−0.10207−0.18020.07819
), ArticleFig(id=1320889313483670403, tenantId=1146029695717560320, journalId=1260987677001138203, articleId=1320889305627738921, language=EN, label=Table 4, caption=

Calculation results of all-E astaxanthin, 9-Z, 13-Z and 15-Z-astaxanthin and transition states of three Z isomers by unrestricted open shell (S2)

, figureFileSmall=null, figureFileBig=null, tableContent=
AST构型S2
全反式2.0984
9顺式2.0971
13顺式2.0992
15顺式2.0984
9顺式过渡态2.1446
13顺式过渡态2.1515
15顺式过渡态2.1499
), ArticleFig(id=1320889313966015365, tenantId=1146029695717560320, journalId=1260987677001138203, articleId=1320889305627738921, language=CN, label=表4, caption=

全反式、9顺式、13顺式和15顺式和三种顺式AST过渡态的无限制开壳层计算结果(S2)

, figureFileSmall=null, figureFileBig=null, tableContent=
AST构型S2
全反式2.0984
9顺式2.0971
13顺式2.0992
15顺式2.0984
9顺式过渡态2.1446
13顺式过渡态2.1515
15顺式过渡态2.1499
), ArticleFig(id=1320889314041512838, tenantId=1146029695717560320, journalId=1260987677001138203, articleId=1320889305627738921, language=EN, label=Table 5, caption=

Three kinds of tunneling correction between Wigner method a and Skodje-Truhlar method b

, figureFileSmall=null, figureFileBig=null, tableContent=
过程隧道效应校正a速率常数隧道效应校正b速率常数
全反式⇌9顺式1.0112.6031×1031.0112.6034×103
全反式⇌13顺式1.0062.7778×1051.0062.7779×105
全反式⇌15顺式1.0166.3759×1041.0166.3770×104
), ArticleFig(id=1320889314121204615, tenantId=1146029695717560320, journalId=1260987677001138203, articleId=1320889305627738921, language=CN, label=表5, caption=

维格纳法a与Skodje-Truhlar法b的三种相互转换的隧道效应校正

, figureFileSmall=null, figureFileBig=null, tableContent=
过程隧道效应校正a速率常数隧道效应校正b速率常数
全反式⇌9顺式1.0112.6031×1031.0112.6034×103
全反式⇌13顺式1.0062.7778×1051.0062.7779×105
全反式⇌15顺式1.0166.3759×1041.0166.3770×104
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虾青素光异构化机理:实验与量子化学相结合研究
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周乐松 , 邹晓君 , 陈佳玲 , 肖杰 , 曹庸 , 刘晓娟 *
食品工业科技 | 研究与探讨 2026,47(5): 92-100
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食品工业科技 |研究与探讨 2026 , 47 (5) : 92 -100
虾青素光异构化机理:实验与量子化学相结合研究
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周乐松 , 邹晓君, 陈佳玲, 肖杰, 曹庸, 刘晓娟*
作者信息
  • 华南农业大学食品学院,广东省功能食品活性物重点实验室,广东广州 510642
通讯作者:
刘晓娟(1980−),女,博士,教授,研究方向:功能食品学、食品生物化学及营养学,E-mail:。
作者简介:

周乐松(1998−),男,硕士研究生,研究方向:功能食品学,食品生物化学及营养学,E-mail:

Mechanism of Photoisomerization of Astaxanthin: Experimental and Quantum Chemistry Study
Lesong ZHOU , Xiaojun ZOU, Jialing CHEN, Jie XIAO, Yong CAO, Xiaojuan LIU*
Affiliations
  • College of Food Science, South China Agricultural University, Guangdong Provincial Key Laboratory of Nutraceuticals and Functional Foods, Guangzhou 510642, China
出版时间: 2026-03-01 doi: 10.13386/j.issn1002-0306.2025020096
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为探究虾青素(astaxanthin,AST)的光异构化机理,采用HPLC技术和Q值法分析光催化转化AST的顺式构型种类和含量,通过密度泛函理论对AST构型进行优化与频率分析,计算得到全反式(all-E)和顺式(Z)AST相互转化的热力学、动力学和能量参数。结果表明,全反式AST在光催化下主要形成9顺式(9-Z)和13顺式(13-Z),13-Z含量(17.72%)显著高于9-Z(13.57%)(P<0.05)。光照后,中性AST分子形成双自由基,双键容易发生扭转。全反式AST的前线轨道能隙差最小,更容易从基态转变为激发态,从而异构为其它构型;根据吉布斯自由能,AST异构体的相对稳定性顺序为:全反式>9-Z>13-Z>15-Z,与实验结果趋势基本相符;全反式AST形成9-Z的活化能高于15-Z和13-Z,单顺式AST转化为多顺式的活化能远高于全反式AST转化为单顺式异构体;13-Z构型生成速率分别约为15-Z和9-Z的4倍和100倍,且相互转化的隧穿效应可以忽略不计,与实验中多顺式异构体难以观察到相吻合,同时阐明实验中出现的13-Z AST比例显著高于9-Z的原因。研究结果揭示了AST可控实现异构体的生成机制,同时为其它类胡萝卜素异构化研究提供理论基础。

虾青素  /  异构化  /  量子化学  /  全反式异构体  /  顺式异构体

To investigate the photoisomerization mechanism of astaxanthin (AST), the types and contents of Z-configuration in photocatalytic conversion of AST were analyzed by HPLC and Q value method. Additionally, the AST configuration was optimized and frequency analysis was performed using density functional theory (DFT). Thermodynamic, kinetic, and energetic parameters of all-E- and Z-AST isomers were further calculated. The results demonstrated that 9-Z- and 13-Z-isomers were predominantly generated under photocatalysis, with the 13-Z content (17.72%) being significantly higher than 9-Z (13.57%) (P<0.05). Upon illumination, neutral AST molecules generated diradicals, facilitating bond twisting. All-E AST exhibited the smallest frontier orbital energy gap, promoting its transition from the ground state to the excited state, and subsequent isomerization into other configurations. Gibbs free energy analysis revealed the following stability order of AST isomers: all-E>9-Z>13-Z>15-Z, basically consistent with experimental observations. Moreover, the activation energy for all-E→9-Z conversion was higher than for all-E→15-Z/13-Z, while single-Z→double-Z isomerization required significantly higher energy than all-E→mono-Z conversion. Notably, the 13-Z-isomer formation rate was about 4-fold and 100-fold higher than that of 15-Z> and 9-Z, respectively. The negligible tunneling effect during mutual transformation explained the scarcity of multi-Z-isomers in experiments and the predominance of 13-Z over 9-Z AST. Collectively, these findings elucidate the controlled generation mechanism of AST isomers and establish a theoretical framework for carotenoid isomerization.

astaxanthin  /  isomerization  /  quantum chemistry  /  all-E-isomer  /  Z-isomer
周乐松, 邹晓君, 陈佳玲, 肖杰, 曹庸, 刘晓娟. 虾青素光异构化机理:实验与量子化学相结合研究. 食品工业科技, 2026 , 47 (5) : 92 -100 . DOI: 10.13386/j.issn1002-0306.2025020096
Lesong ZHOU, Xiaojun ZOU, Jialing CHEN, Jie XIAO, Yong CAO, Xiaojuan LIU. Mechanism of Photoisomerization of Astaxanthin: Experimental and Quantum Chemistry Study[J]. Science and Technology of Food Industry, 2026 , 47 (5) : 92 -100 . DOI: 10.13386/j.issn1002-0306.2025020096
虾青素(3,3′-二羟基-4,4′-二酮基-β,β′-胡萝卜素,astaxanthin,AST)是一类脂溶性酮式类胡萝卜素,由于其强大的抗氧化、抗炎、提高免疫以及着色能力,在医药、保健食品、化妆品以及养殖领域广泛使用[1−4]。AST的结构中包含2个β-紫罗兰酮环以及11个共轭双键,加热或光照下双键扭转使得AST产生多种异构体,如全反式(all-E)、9顺式(9-Z)和13顺式(13-Z)等。近年来的研究表明,全反式AST在加热、光照、高压、微波以及添加催化剂等作用下实现向顺式异构体的转化[5]。最新研究报道,富含顺式异构体的AST发挥更强的健康效应,如抗衰老、抗炎、降脂等[6−7]。因此,类胡萝卜素(包括AST)顺式异构化的形成过程和机制逐渐受到关注,尽管已有一些初步研究,但具体机理仍需进一步探讨和验证。
类胡萝卜素异构化过程仍存在共性的难题有待阐明,如全反式向顺式构型转化的具体路径,转化后的终产物,以及转化过程需要的反应条件等,上述关键环节的机理缺失制约了人们对类胡萝卜素异构化过程的系统性理解。同样,现有的技术水平阻碍了AST顺式异构体形成机理的揭示。目前,AST异构体的检测主要结合高效液相色谱(high performance liquid chromatography,HPLC)以及二极管阵列检测器,对全反式AST的异构化产物进行定性和定量分析[8]。但是AST异构化中产生的痕量中间体却难以捕获,为了鉴定AST的异构化过程中的中间产物,需要结合高分辨率仪器,如超高分辨率质谱等进行分析[9]。由于中间体结构相似,难以分离和纯化,因此AST顺式转化机理还有待进一步探索。
量子化学在类胡萝卜素领域的应用在过去二十年中获得了关注,通过分子轨道理论、价键理论、溶剂化模型、势能面理论等量化方法可以得到类胡萝卜素各种反应的计算参数。以往量子化学计算报道集中于类胡萝卜素与蛋白结合后或聚集状态下光谱的变化、类胡萝卜素自由基与金属离子结合的能量变化、类胡萝卜素抗氧化活性研究等[10−11]。对于类胡萝卜素异构化机理研究仍有很大探索空间。利用量子化学揭示类胡萝卜素异构化过程的工作主要从β-胡萝卜素开始,Guo等[12]利用密度泛函理论在B3LYP/6-31G(d)水平上对开壳层(一个以上亚层未充满的电子组态)单重态和三重态β-胡萝卜素进行计算。通过比较不同β-胡萝卜素异构体分子的能量,证明了β-胡萝卜素异构体的稳定性顺序为:全反式>9顺式>13顺式>15顺式。此外,他们还揭示了13顺式β-胡萝卜素的旋转势垒能量最低。以往的研究虽然计算了不同类胡萝卜素异构体的能垒,但并未采用量子化学结合实验对类胡萝卜素进行分析,同时也未进一步分析类胡萝卜素异构化过程的结构变化、能量变化以及速率变化等。
基于此,为揭示AST的光异构化机理,包括顺式异构体生成类型及其原因,本研究采用HPLC和Q值法分析AST光催化转化的顺式构型种类和含量,在B3LYP/6-31G(d)水平上计算研究全反式(all-E)和顺式(Z)AST相互转化的热力学参数、前线轨道、活化能和转化速率,同时利用量子化学理论揭示光催化转化实验的异构化现象。本研究有望揭示AST可控实现异构体的生成机制,以期为其它类胡萝卜素异构化研究提供理论依据。
全反式AST(纯度>99%) 广东巨元生化有限公司;顺式AST(纯度为31.30%,其中9顺式和13顺式分别为13.57%和17.73%)、9顺式AST(纯度为88.31%)、13顺式AST(纯度为95.68%) 实验室制备;二氯甲烷(分析纯)、无水乙醇(分析纯) 天津富宇精细化工有限公司;碘(分析纯) 天津福晨化学试剂有限公司。
LC-15C高效液相色谱仪(配有二极管阵列检测器) 日本岛津公司;RE212旋转蒸发仪 上海亚荣生化仪器厂;LED灯 温州蔚来电气技术有限公司。
称量200 mg全反式AST溶解于100 mL二氯甲烷中,在25 ℃温度条件下,放置于LED灯下(光强150 lx,波长范围450~465 nm)光照搅拌10 min,进行全反式AST光异构化,得到含一定顺式比例的AST固体粉末,即光异构化AST。然后用无水乙醇溶解光异构化AST,超声悬浮,放置于4 ℃冰箱静置2 h,以4000 r/min离心20 min,去除沉淀后,用0.22 μm聚四氟乙烯有机系滤膜过滤后,旋蒸至干,将Z-AST粗提样放置于−20 ℃保存。
接下来采用200~300目硅胶粉进行柱层析,配制正己烷/二氯甲烷/甲醇(100/200/3,v/v)洗脱剂,用二氯甲烷溶解Z-AST初提样,以3.5 mL/min流速匀速洗脱,取不同分离时间段样品,进行薄层色谱法分析。根据硅胶板上的比移值,合并收集后氮吹,得到9顺式和13顺式AST。
取上述光异构化AST,全反式以及制备得到的9顺式和13顺式AST样品分别加入4.95 mL二甲基亚砜(dimethyl sulfoxide,DMSO)溶解,DMSO不会造成AST降解及构型改变[13]。HPLC检测条件为:流动相A相为一级水,流动相B相为甲醇/乙腈/二氯甲烷(85/5/5,v/v)的混合溶液。A相比例5%,B相为95%,流速为1 mL/min。进样量20 μL,运行时间为20 min,柱温为25 ℃,紫外检测器波长为476 nm,采用等度洗脱方式对AST及其异构体进行检测。
根据HPLC保留时间,HPLC二极管阵列检测器生成的电子吸收光谱中顺式峰(约360 nm)与异构体的主要吸收峰的相对强度相比,得到Q值,鉴定全反式、顺式AST、9顺式AST、13顺式AST。通过对HPLC图谱476 nm处峰面积积分对AST异构体进行定量分析。
顺式AST含量(%)计算公式如下:
$ 顺式\text{AST}含量(\text{%})=\frac{顺式\text{AST}总面积}{\text{AST}总面积}\times \text{100} $
计算步骤:B3LYP方法是一种混合泛函,由贝克(Becke)的三重杂化泛函、李-杨(Lee-Yang)-帕尔(Parr)的局部密度近似(local density approximation,LDA)、恩泽霍夫(Ernzerhof)的梯度修正三个部分构成[14−15]。在以往报道中,B3LYP/6-31G(d)基组已被证明计算类胡萝卜素的旋转势垒是可靠的。参考Guo等[12]的做法并加以改进,通过Gauss view 6.0软件在气相(真空)条件下中构建全反式、9顺式、13顺式、15顺式AST中性分子与双自由基的分子模型,AST分子的自由基形态由自旋多重度控制,中性分子与双自由基的自旋多重度均设置为1。
在密度泛函(density functional,DFT)法的B3LYP/6-31G(d)基组水平下对其构型进一步优化与频率分析,结果振动频率无负值,虚频为零,得到完全优化的稳态点的吉布斯自由能。考虑到溶剂对AST异构化的影响,使用极化连续介质模型(polarized continuum model,PCM)的二氯甲烷,并在密度泛函法(DFT法)的B3LYP/6-311++G(d,p)基组水平下,温度设置为298.15 K(25 ℃)计算得到单点电子能。加上在真空条件下优化与频率分析得到的吉布斯自由能进行热修正,得到了参与电荷转移反应的各物质的绝热吉布斯自由能,同时在密度泛函法(DFT法)的B3LYP/6-311++G(d,p)基组水平下计算前线轨道能。
计算使用密度泛函理论(DFT)、极化连续介质模型(PCM)均在高斯16(Gaussian 16)和Gaussview 6.0中实现[16]。在相同温度条件下,通过Shermo程序计算热力学数据,并导入TST calculator计算AST异构化反应速率常数[17−18]。
每组实验重复测定三次,结果表示为平均值±标准差。利用软件SPSS22.0对实验数据进行显著性分析,P<0.05为差异显著,使用Origin绘制图像。
天然来源的AST大多为全反式构型,异构化需要光或热的形式提供能量,从而打断共轭双键中彼此连贯重叠形成的离域π键,因此光和热成为影响AST异构化的主要因素[19]。如图1A为全反式AST光异构化的HPLC色谱图,根据AST异构体的出峰保留时间(图1B~D)和纯化后各峰电子吸收图谱的Q值(图1E~G),即顺式峰的吸光度与主峰吸光度的比值,结合以往文献报道[8,20],进一步鉴定峰1、峰2和峰3分别为全反式(all-E)、9顺式(9-Z)和13顺式(13-Z)AST(表1)。由此可见,全反式AST在光照作用下异构化主要生成9顺式和13顺式构型,其含量分别为13.57%和17.72%。然而,通过实验手段难以阐明AST顺式化的优选途径,因此后续借助量子化学手段来揭示AST顺式异构化机理。
通常认为类胡萝卜素顺式几何异构体的形成,是通过单线态双自由基介导进行的,全反式构型在形成双自由基后,经过介于单键与双键的新形成键的旋转,形成不同顺式异构体[21]。类胡萝卜素通过调节自旋多重度来生成非自由基态(中性分子)和自由基态(如双自由基),因此,构建AST中性分子和双自由基结构,并在此基础上进行量化计算[22]。
全反式和顺式AST的中性和双自由基优化结构如图2所示,并在此基础上计算吉布斯自由能(Gibbs free energy)(表2)。吉布斯自由能为化学热力学中判断过程进行的方向而引入的热力学函数[23]。中性分子在化学反应中通常不直接参与电荷转移,因为它们不带电荷,所以在自然状态下,AST均为基态,即中性分子。中性分子中,AST吉布斯自由能的大小顺序为:15顺式>13顺式>9顺式>全反式(分子结构如图3)。在热力学上,全反式是AST最稳定的异构体,9顺式相较其它两种顺式稳定,15顺式为最不稳定的异构体,因此实验以及自然界中主要观察到9顺式和13顺式。双自由基指一个体系里有两个未成对电子,它们的自旋相反,为单重态体系。在光照作用下,AST跃迁到激发态,即单重态参与异构化反应,因此双自由基形式的AST是异构化的初始形态。在双自由基状态下,双键获得了类似普通键(介于单键和双键之间的共价键)的性质,围绕键的旋转使得激发态全反式和顺式AST之间相互转换,因此进一步分析双自由基能量可以判断异构化方向。由表2可知,9顺式双自由基能量高于全反式,13顺式和15顺式双自由基能量远低于全反式,说明9顺式双自由基是最不稳定的自由基,极有可能在光照作用下进一步异构化。理论上激发态的9顺式AST反应性最高,但在初始反应体系中,以激发态的全反式AST为主,因此激发态的全反式AST异构为9顺式后,可能顺式异构化为双顺式异构体。在光照过程中,AST从基态跃迁至激发态,即从中性分子转化为双自由基,但双自由基不稳定,除了进行上述的异构化反应,也可以通过发射荧光回到中性分子。
键长和二面角ζ是影响AST分子稳定性的关键因素,因此接下来进一步对这两个参数进行分析。如图4所示,由于受到π电子离域的影响,AST异构体主链上的C-C单键计算出的所有键长均小于1.53Å(普通烷烃的单键键长)[24];全反式AST从中性分子跃迁至双自由基过程中,由图4统计的键长可知,双键的长度增加0.05~0.08Å,单键减少0.06~0.09Å,改变了单双键的键长。由于键长的变化,使得AST更容易产生键的扭转。此外,顺反AST形成双自由基后,弯折处二面角ζ均发生一定变化,全反式AST增加0.003~0.007°;9顺式、13顺式和15顺式AST的二面角ζ分别增加0.2°、0.9°和1.5°,二面角ζ的变化可能影响稳定性,15顺式AST的二面角ζ变化最大,越不稳定。由图4共轭双键拐角处可知,二面角ζ的角度均在178~179°,由于幅度较小,具体稳定性需要实验进一步验证。
以上结果表明,在光作用下,全反式AST分子形成激发态(双自由基态),键更容易扭转,形成顺式构型;从能量角度上看,9顺式AST激发态更不稳定,可能进一步转化;从结构角度上,15顺式AST激发态难以存在;基态分子中,全反式AST最稳定,9顺式和13顺式稳定性高于15顺式。因此自然界中以全反式异构体为主,且光异构化后主要生成9顺式和13顺式异构体。
接下来进一步采用前线轨道理论分析AST分子的稳定性。前线轨道理论将分子周围分布的电子云根据能量细分为不同能级的分子轨道,能量最高的分子轨道(最高占据轨道,highest occupied molecular orbital,HOMO)和没有被电子占据的、能量最低的分子轨道(最低未占轨道,lowest unoccupied molecular orbit,LUMO)是决定一个体系发生化学反应的关键,分子发生反应的难易程度也决定了物质的稳定性[25]。进行化学反应时,电子从最高占据分子轨道HOMO流入最低未占有分子轨道LUMO,且电子从分子中电负性小的元素流向电负性大的元素。从图5可以看出,AST的共轭长链、羟基和酮基上均分布有分子轨道,因此,电子云主要分布在碳碳双键、羟基和酮基上[26]。
由2.2可知,电子由HOMO跃迁至LUMO的过程,主要发生在AST的共轭双键上,如图5,AST的直链共轭多烯呈现单键、双键交替分布,左图AST在基态(S0)状态下时,HOMO能级下分子轨道主要分布在碳碳单键的位置,具有电子给予体的性质;右图在激发态(S1)下,LUMO能级下主要在碳碳双键,具有电子接受体的性质。凡含有双键的不饱和有机化合物,均产生π到π*的跃迁(基态→激发态),以实现成键π电子由基态跃迁到π*轨道。更进一步说,AST在光照作用下伴随着基态(S0)向激发态(S1)的跃迁,HOMO-LUMO能隙是AST中性分子中电子激发所需的最小能量。AST从中性分子转变为双自由基这一过程,侧面反映了AST异构体的光稳定性,能隙越小,越容易被激发[27−28]。通过表3可知,AST异构体的能隙大小顺序为:全反式<9顺式<15顺式<13顺式,这意味着全反式AST容易转化为其它顺式异构体,13顺式AST在光照作用下相对稳定,不容易回复异构化。
以上结果表明,在光照作用下,HOMO-LUMO能隙决定AST实现从基态到激发态跃迁的难易程度,全反式构型的能隙最小,相较其它顺式异构体更容易从基态跃迁到激发态,反应性最高,13顺式构型则相反。
由于双自由基形式的AST是异构化的初始形态,在2.2对AST分子构型优化的基础上,进一步分析了全反式AST异构化过程中生成单顺式、双顺式异构体的难易程度。类胡萝卜素异构化的过程中,分子结构发生改变,需要跨过一定能垒才能完成反应。能垒的高度表示反应物变成产物所必须克服的能量障碍大小,能垒越高,越难生成活化的中间产物,即过渡态(TS)(transition state,TS)[29]。活化能是对能垒的一种量化描述,代表着反应物到过渡态的具体能量差值。通过分析过渡态结构和能垒,可以描述物质异构化的过程[30]。研究表明将全反式叶黄素在光照作用下转化为顺式异构体的不同活化能(Ea)存在差异,从而导致异构体产生比例不同[31]。
首先,对双自由基体系反应过程的可靠性进行考察。对于自由基体系,过渡金属配合物等均需要进行不受限制开壳计算,以便考察单电子(不成对的电子)分布。由于AST光照异构化的过程是在双自由基基础上进行,双自由基理论计算使用不受限制开壳计算,在此计算过程中有两组相同的自旋轨道(α电子和β电子),两组轨道基函数相同,但分子轨道参数不同。当α和β自旋轨道的空间部分不同时,不希望出现具有高度自旋污染的近似波函数,避免自旋造成计算的总能量的升高或降低[32]。S2值常被用来衡量自旋污染程度,S2的结果见表4。对于自旋多重度为1的双自由基AST,该值应为2。经计算,自旋污染与2偏差值在4.85%~7.57%范围内,小于10%。因此,自旋污染不严重,可以忽略,计算结果可靠[29]。
全反式AST异构化的过程伴随着化学键的断裂与生成,随着新的化学键沿着二面角扭转,往往伴随着过渡态以及中间体生成[33]。2.2描述全反式AST在光照作用下双键断裂,生成普通键,形成双自由基。因此以全反式AST双自由基为起始几何构型,分别沿着C29-C27-C31-C29,C39-C37-C41-C43,C42-C44-C43-H95二面角旋转得到9顺式、13顺式和15顺式AST的势能分布图。势能面反映出整个化学反应过程的全貌以及反应的始终态、中间体和过渡态的基本态势,如图6所示,内禀反应坐标(IRC)是连接势能面相邻两个极小点的能量最低路径,描述了化学过程在不考虑热运动因素下最理想的结构变化轨迹[34]。IRC沿着势能面最低的点将反应物与产物之间能量连接起来。两个峰代表过渡态(TS),频率是过渡态的判定标准,顺反异构化的TS结构及其虚频率如图7、图8所示,为验证过渡态,经频率计算,只有一个虚的(负的)频率;曲线的谷代表中间体,势能面上的最高点与最低点的差值即为能垒,同时图中给出全反式AST与AST过渡态能量之差即为全反式AST转变为不同顺式异构体的能垒。经测定,三种过渡态的扭转角分别为75.01°、90.09°和90.06°,当扭转角与109.5°相差越大,趋势越大,角张力越大,结构越不稳定,因此9顺式AST过渡态为最不稳定构型[35]。全反式AST通过9顺式过渡态、15顺式过渡态和13顺式过渡态转化为顺式异构体的能垒能量分别为12.8、10.9和10.0 kcal/mol,返回路径的势垒能量分别为11.5、7.1和7.4 kcal/mol。由图6可知,能垒大小顺序为:9顺式>15顺式>13顺式AST,因此双自由基形态的9顺式AST最难形成,13顺式生成速率快,同时返回路径的势垒也低,更容易回复形成全反式。
在比较单顺式AST生成难易的同时,进一步考虑双顺式AST生成的可能性。由上文2.2的双自由基能量分析以及2.3的HOMO−LUMO能隙可知,9顺式AST双自由基的反应性高于全反式,中性分子状态下仅次于全反式,因此9顺式AST可能进一步形成双顺式,因此以其双自由基形态为起始几何构型,分别沿着C30-C28-C32-C34,C39-C37-C41-C43和C42-C44-C43-H95二面角旋转得到9,9’、9,13、9,15-双顺式异构体的势能面分布,三种双顺式AST过渡态如图8所示,旋转能垒能量分别为13.0、10.1和10.8 kcal/mol,远远高于单顺式AST回复异构化所需能量,这部分能量足以使得单顺式AST回复异构化为全反式 AST,这与Zhang等[36]将高比例顺式AST在光照下回复为全反式AST的实验结果一致。同时理论证明了番茄红素多顺式异构体可以由较高活化能Ea的单顺式异构体产生,但多顺式构型的番茄红素能垒足以使得单顺式构型回复至全反式[37]。
除了考察不同AST的能垒,异构化反应速率也是决定异构化终产物的关键因素。AST的异构化遵循一阶反应动力学,初始阶段的异构化反应可以近似用零级反应动力学(反应速率与反应物的浓度无关)表示[20]。因此利用速率模型对异构化过程进行计算,基于过渡态(TS)理论估计的相互转换速率对AST单分子顺反动力学速率常数进行测定,如表5,计算结果得到13顺式AST转化速率远高于9顺式、15顺式,全反式AST向13顺式AST的转化速度分别约为15顺式、9顺式AST的4倍和100倍。由于全反式和13顺式AST相互转化的速率常数最高,9顺式AST相互转化的速率常数最低,因此长时间的光照会使得13顺式AST回复异构化,9顺式AST比例上升较慢,可能会导致两种异构体的比例相当。
以上结果表明,在光照作用下,全反式AST形成双自由基,且生成的双自由基9顺式AST最不稳定;生成13顺式构型的能垒最低,反应速率最快,为9顺式构型反应速率的100倍,生成双顺式构型需要极高能垒,因此光异构化主要生成单顺式异构体。由于低能垒中间体返回路径的能垒同样降低,异构速率快的顺式构型也容易回复为全反式,使得两种顺式构型比例相当。全反式AST的稳定性高于顺式AST,与文献报道结果一致,由于稳定性测定方式不同,不同顺式异构体的稳定性略有差异[38−39]。全反式AST光异构化机理示意图如图9。
本研究结合实验方法和量子化学理论阐明了全反式AST光异构化机理。AST在光照作用下主要生成9顺式和13顺式;全反式AST光异构化机理为:由于全反式AST的前线轨道能隙差最小,更容易受到光照激发转化为双自由基,双自由基形态全反式AST的双键具备类似普通键的性质,扭转的能垒降低,即活化能降低,容易转变为顺式构型,生成顺式构型后,通过发射荧光回到中性分子。吉布斯自由能可知,AST异构体中性分子形态的相对稳定性顺序为:全反式>9顺式>13顺式>15顺式,因此9顺式和13顺式稳定存在。单顺式AST转化生成双顺式的活化能远高于全反式AST转化为单顺式异构体,因此实验中主要观察到单顺式异构体。由于能垒的差异,全反式AST向13顺式的转化速率分别约为15顺式、9顺式AST的4和100倍,且相互转化的隧穿效应可以忽略不计,9顺式、13顺式的速率与实际实验结果相印证。因此,由于AST异构体前线轨道能隙、分子能量、能垒和异构速率差异,全反式AST光照过程中主要生成单顺式,尤其是13顺式AST。后续将进一步采用实验和量子化学相结合手段揭示AST的其它顺式异构化机理,如加热、高压、微波等。研究结果为揭示类胡萝卜素顺式异构化提供理论依据和应用指导价值。

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2026年第47卷第5期
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doi: 10.13386/j.issn1002-0306.2025020096
  • 接收时间:2025-02-17
  • 首发时间:2026-10-24
  • 出版时间:2026-03-01
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  • 收稿日期:2025-02-17
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    华南农业大学食品学院,广东省功能食品活性物重点实验室,广东广州 510642

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刘晓娟(1980−),女,博士,教授,研究方向:功能食品学、食品生物化学及营养学,E-mail:。
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2种不同金属材料的力学参数
科
Family
属数
Number of
genus
种数
Number of
species
占总种数比例
Percentage of
total species (%)
属
Genus
种数
Number of
species
占总种数比例
Percentage of total
species (%)
鹅膏菌科Amanitaceae 2 11 5.26 鹅膏菌属 Amanita 10 4.78
小菇科 Mycenaceae 2 12 5.74 丝盖伞属 Inocybe 5 2.39
多孔菌科 Polyporaceae 8 14 6.70 蜡蘑属 Laccaria 5 2.39
红菇科 Russulaceae 3 23 11.00 小皮伞属 Marasmius 6 2.87
小菇属 Mycena 11 5.26
光柄菇属 Pluteus 5 2.39
红菇属 Russula 17 8.13
栓菌属 Trametes 5 2.39
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