Yamada H, Hieda K
Biophysics Laboratory, College of Science, Rikkyo University, Tokyo, Japan.
Photochem Photobiol. 1992 Apr;55(4):541-8. doi: 10.1111/j.1751-1097.1992.tb04276.x.
The action cross sections for the formation of the cyclobutane dimer and the (6-4) photoproduct of thymine as well as the absorption cross sections of thymine were determined in the wavelength region between 150 and 290 nm. Thymine films sublimed on glass plates were irradiated by monochromatic photons in a vacuum; the induced photoproducts were quantitatively analyzed by high-performance liquid chromatography (HPLC). Under our conditions, two major peaks appeared on the HPLC chromatograms of irradiated samples. The two peaks were identified as being the cis-syn cyclobutane dimer and the (6-4) photoproduct, based on their HPLC retention times, absorption spectra in the effluent, and photochemical reactivity. The fractions of the two photoproducts increased linearly with the fluence at low fluences over the entire wavelength range. Their action cross sections were determined by the slopes of the linear fluence response curve at 10 nm intervals between 150 and 290 nm. The two action spectra showed a similar wavelength dependence and had a maximum at 270 nm as well as two minor peaks at 180 and 220 nm, at which wavelengths the peaks of the absorption spectrum of thymine sublimed on a CaF2 crystal plate appeared. The quantum yields had relatively constant values of around 0.008 for the dimer and 0.013 for the (6-4) photoproduct above 200 nm, decreasing to 0.003 and 0.006, respectively, at 150 nm as the wavelength became shorter.
在150至290纳米的波长范围内,测定了胸腺嘧啶形成环丁烷二聚体和(6 - 4)光产物的作用截面以及胸腺嘧啶的吸收截面。在真空中,用单色光子照射升华在玻璃板上的胸腺嘧啶薄膜;通过高效液相色谱法(HPLC)对诱导产生的光产物进行定量分析。在我们的实验条件下,辐照样品的HPLC色谱图上出现了两个主要峰。根据它们的HPLC保留时间、流出物中的吸收光谱以及光化学反应性,这两个峰被鉴定为顺式 - 顺式环丁烷二聚体和(6 - 4)光产物。在整个波长范围内,在低通量时,这两种光产物的分数随通量呈线性增加。它们的作用截面由150至290纳米之间以10纳米间隔的线性通量响应曲线的斜率确定。这两个作用光谱显示出相似的波长依赖性,在270纳米处有一个最大值,在180和220纳米处有两个较小的峰,在这些波长处,升华在CaF2晶体板上的胸腺嘧啶吸收光谱出现峰值。在200纳米以上,二聚体的量子产率相对恒定,约为0.008,(6 - 4)光产物的量子产率约为0.013,随着波长变短,在150纳米处分别降至0.003和0.006。