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卟啉及其衍生物的结构和振动电子特性的比较研究。

Comparative study of the structural and vibroelectronic properties of porphyrin and its derivatives.

作者信息

Aydin Metin

机构信息

Department of Chemistry, Faculty of Art and Sciences, Ondokuz Mayıs University, Samsun 55139, Turkey.

出版信息

Molecules. 2014 Dec 15;19(12):20988-1021. doi: 10.3390/molecules191220988.

DOI:10.3390/molecules191220988
PMID:25517340
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC6271358/
Abstract

Density functional theory (DFT and time-dependent-DFT (TD-DFT) were employed to investigate the vibroelectronic structural properties of porphyrin and some derivatives: unsubstituted porphyrin (TPyr), meso-tetraphenylporphyrin (TPP), meso-tetrakis(p-sulfonatophenyl)porphyrin (TSPP), protonated-TPyr (H2TPyr), deuterated-H2TPyr (D4TPyr), protonated-TPP (H2TPP) and deuterated-H2TPP (D4TPP), protonated TSPP (H2TSPP), deuterated-H2TSPP (D4TSPP), dicationic TSPP (H6TSPP) and deuterated-H6TSPP (D8TSPP). The possible internal conversion (IC) and intersystem crossing (ISC) processes of these compounds were investigated. Finally, the relaxed ground state potential energy surface (PES) (S0), and singlet (Sn, n = 1-24) and triplet (Tn) excited state PESs of the TSPP molecule were calculated as function of the dihedral angle (Cα-Cm-Cϕ-C(ph)) rotation. The results of the calculations indicated that while the meso-substitutions caused a significant shift in frequencies when the meso-carbons within the parent-porphine (or TPyr) are involved in the vibrational motion of molecules; the protonation of the N atoms at the porphine/porphyrin core causes a significant blue shift when the H on the N atoms within the pyrroline are dominantly involved in the vibrational motions. The deuteration of N atoms not only caused a red-shift in the frequencies of the corresponding peaks below 1600 cm(-1), but also produced new vibrational modes of frequencies in the 2565-2595 cm(-1) range caused by the N-D bond stretching. Similarly, the deuteration of O atoms within the sulfonato groups (-SO3(-)) exhibited a new peak at around 2642 cm(-1) due to O-D bond stretching. The measured Raman spectrum of the H2TSPP is assigned based on the predicted Raman spectra of the compounds studied here and measured Raman spectrum of the TPP (from our previous work). The IR spectrum is assigned based on our calculations and measured IR spectra obtained from the literature. The results of the TD-DFT calculations did not only indicate that the meso-substitution and protonation of the porphyrin bring about a significant read shift in the electronic transitions; but also provided a strong evidence for the IC from the Soret band to Q-bands beside possibility of the ISC process; its existence depend on the other excited state process such as much faster vibrational relaxation; the IC and etc. The ground state PES curve (S0) of the ionic TSPP exhibited two minima at the dihedral angle (Cα-Cm-Cϕ-C) of about 66° (corresponds to the lowest ground state) and 110° (corresponds to next energetically stable state or the local minima). The energy deference between these two minima is 0.0132 eV (or 106 cm(-1)) and the highest potential energy barrier when undergoing from the lowest ground state to this local state is only 0.0219 eV (177 cm(-1); which is compatible with the thermal energy (kT) at 298 K is 207.2 cm(-1).

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e9e5/6271358/9ed9477f7b02/molecules-19-20988-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e9e5/6271358/e412b90cebda/molecules-19-20988-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e9e5/6271358/cff3e80b69b0/molecules-19-20988-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e9e5/6271358/fd3e57fd7855/molecules-19-20988-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e9e5/6271358/38d58d46ffc7/molecules-19-20988-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e9e5/6271358/b33733e63006/molecules-19-20988-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e9e5/6271358/025d014a9cfb/molecules-19-20988-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e9e5/6271358/9ed9477f7b02/molecules-19-20988-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e9e5/6271358/e412b90cebda/molecules-19-20988-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e9e5/6271358/cff3e80b69b0/molecules-19-20988-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e9e5/6271358/fd3e57fd7855/molecules-19-20988-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e9e5/6271358/38d58d46ffc7/molecules-19-20988-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e9e5/6271358/b33733e63006/molecules-19-20988-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e9e5/6271358/025d014a9cfb/molecules-19-20988-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e9e5/6271358/9ed9477f7b02/molecules-19-20988-g007.jpg
摘要

采用密度泛函理论(DFT)和含时密度泛函理论(TD-DFT)研究了卟啉及其一些衍生物的振动电子结构性质:未取代卟啉(TPyr)、中位四苯基卟啉(TPP)、中位四(对磺酸钠苯基)卟啉(TSPP)、质子化-TPyr(H2TPyr)、氘代-H2TPyr(D4TPyr)、质子化-TPP(H2TPP)和氘代-H2TPP(D4TPP)、质子化TSPP(H2TSPP)、氘代-H2TSPP(D4TSPP)、二价阳离子TSPP(H6TSPP)和氘代-H6TSPP(D8TSPP)。研究了这些化合物可能的内转换(IC)和系间窜越(ISC)过程。最后,计算了TSPP分子的弛豫基态势能面(PES)(S0)以及单重态(Sn,n = 1 - 24)和三重态(Tn)激发态势能面随二面角(Cα-Cm-Cϕ-C(ph))旋转的变化。计算结果表明,当母体卟吩(或TPyr)中的中位碳原子参与分子的振动运动时,中位取代会导致频率发生显著位移;当吡咯啉内氮原子上的H主要参与振动运动时,卟啉/卟啉核上氮原子的质子化会导致显著的蓝移。氮原子的氘代不仅使低于1600 cm(-1)的相应峰频率发生红移,还产生了由N - D键伸缩引起的2565 - 2595 cm(-1)范围内的新振动模式。同样,磺酸根基团(-SO3(-))内氧原子的氘代由于O - D键伸缩在约2642 cm(-1)处出现一个新峰。基于本文研究的化合物的预测拉曼光谱和TPP的测量拉曼光谱(来自我们之前的工作)对H2TSPP的测量拉曼光谱进行了归属。红外光谱基于我们的计算和从文献中获得的测量红外光谱进行了归属。TD-DFT计算结果不仅表明卟啉的中位取代和质子化导致电子跃迁发生显著的红移;还为从Soret带到Q带的内转换以及系间窜越过程的可能性提供了有力证据;其存在取决于其他激发态过程,如更快的振动弛豫、内转换等。离子型TSPP的基态PES曲线(S0)在二面角(Cα-Cm-Cϕ-C)约为66°(对应最低基态)和110°(对应下一个能量稳定态或局部极小值)处呈现两个极小值。这两个极小值之间的能量差为0.0132 eV(或106 cm(-1)),从最低基态转变到该局部态时的最高势能垒仅为0.0219 eV(177 cm(-1));这与298 K时的热能(kT)207.2 cm(-1)是相符的。

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