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全反式视黄醇的光电离与光异裂。溶剂和激光辐射强度的影响。

Photoionization versus photoheterolysis of all-trans-retinol. The effects of solvent and laser radiation intensity.

作者信息

Gurzadyan Gagik G, Reynisson Jóhannes, Steenken Steen

机构信息

Max-Planck-Institut für Bioanorganische Chemie (formerly Max-Planck-Institut für Strahlenchemie), D-45413, Mülheim, Germany.

出版信息

Phys Chem Chem Phys. 2007 Jan 14;9(2):288-98. doi: 10.1039/b609165m. Epub 2006 Nov 21.

Abstract

The time-resolved formation of the retinyl carbocation from all-trans-retinol and all-trans-retinol acetate was studied by use of picosecond flash photolysis. From both precursors, the retinyl cation is produced by heterolytic C-O bond cleavage in solvents of medium polarity (acetonitrile, tetrahydrofuran, propanol with Reichardt polarity parameter ET(N) approximately 0.5) and high polarity (EtOH, MeOH, TFE, HFIP, ET(N) > 0.6) during the laser pulse (< or =5 ps) where its lifetime is >10 ns. The absorption maximum of the cation at early times (t < 100 ps) is at lambda = 590-600 nm; it shifts to shorter wavelengths (Deltalambda = 5-10 nm) within 1-10 ns. This spectral shift is suggested to be due to contact ion pair --> solvent-separated ion pair --> free-ion transformation. The quantum yield of cation formation phi(cat) is independent of excitation wavelength (213, 266 or 355 nm). Photoheterolysis proceeds via a one-quantum process. In chlorinated solvents, i.e. n-BuCl, 1,2-dichloroethane, chloroform or CCl(4), formation of the retinol radical cation (which is characterized by a peak at 610 nm and further absorption maxima at approximately 840 and approximately 940 nm) by intermolecular electron transfer to the solvent molecules was detected. The radical cation lifetime in all these solvents is 1.5-2 ns, except for CCl(4) where it is 0.25 ns. The formation of the radical cation or cation was not detected in the low polarity solvents: cyclohexane, hexane, dioxane and p-xylene. However, in solvents of medium and high polarity, at high radiation intensities the radical cation may form in addition to the cation (as a result of two-quantum ionization). DFT calculations confirm our experimental results. The rate of retinol S(1) depopulation (k = 0.3-1 x 10(9) s(-1)) is almost independent of the solvent polarity in the range from cyclohexane to methanol. In highly polar solvents (ET(N) > 0.9) the rate increases to (0.5-5) x 10(10) s(-1).

摘要

利用皮秒闪光光解研究了全反式视黄醇和全反式视黄醇乙酸酯生成视黄基碳正离子的时间分辨过程。在激光脉冲期间(≤5皮秒),从中等极性(乙腈、四氢呋喃、具有赖夏德特极性参数ET(N)约为0.5的丙醇)和高极性(乙醇、甲醇、三氟乙醇、六氟异丙醇,ET(N)>0.6)的溶剂中,通过异裂C-O键断裂,由这两种前体生成视黄基碳正离子,其寿命>10纳秒。早期(t<100皮秒)碳正离子的吸收最大值在λ=590 - 600纳米处;在1 - 10纳秒内它会向较短波长移动(Δλ = 5 - 10纳米)。这种光谱移动被认为是由于接触离子对→溶剂分隔离子对→自由离子的转变。碳正离子形成的量子产率φ(cat)与激发波长(213、266或355纳米)无关。光异裂通过单量子过程进行。在氯化溶剂中,即正丁基氯、1,2 - 二氯乙烷、氯仿或四氯化碳中,检测到通过分子间电子转移到溶剂分子形成视黄醇自由基阳离子(其特征是在610纳米处有一个峰,在约840纳米和约940纳米处还有进一步的吸收最大值)。除了四氯化碳中自由基阳离子寿命为0.25纳秒外,在所有这些溶剂中自由基阳离子的寿命为1.5 - 2纳秒。在低极性溶剂:环己烷、己烷、二氧六环和对二甲苯中未检测到自由基阳离子或碳正离子的形成。然而,在中等极性和高极性溶剂中,在高辐射强度下,除了碳正离子外可能还会形成自由基阳离子(由于双量子电离)。密度泛函理论计算证实了我们的实验结果。视黄醇S(1)去布居的速率(k = 0.3 - 1×10⁹秒⁻¹)在从环己烷到甲醇的范围内几乎与溶剂极性无关。在高极性溶剂(ET(N)>0.9)中,速率增加到(0.5 - 5)×10¹⁰秒⁻¹。

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