Zipfel E, Grezes J R, Seiffert W, Zimmermann H W
Histochemistry. 1981;72(2):279-90. doi: 10.1007/BF00517141.
Azure B is the most important Romanowsky dye. In combination with eosin Y it produces the well known Romanowsky-Giemsa staining pattern on the cell. Usually commercial azure B is strongly contaminated. We prepared a sample of azure B-BF4 which was analytically pure and had no coloured impurities. The substance was used to redetermine the molar extinction coefficient epsilon (v)M of monomeric azur B in alcoholic solution. In the maximum of the long wavelength absorption at v = 15.61 kK (lambda = 641 nm) the absorptivity is epsilon (15.61)M = (9.40 +/- 0.15) x 10(4)M-1 cm-1. This extinction coefficient may be used for standardization of dye samples. In aqeuous solution azur B forms dimers and even higher polymers with increasing concentration. The dissociation constant of the dimers, K = 2,2 x 10(-4)M (293 K), and the absorption spectra of pure monomers and dimers in water have been calculated from the concentration dependence of the spectra using an iterative procedure. The molar extinction coefficient of the monomers at 15.47 kK (646 nm) is epsilon (15.47)M = 7.4 x 10(4)M-1 cm-1. The dimers have two long wavelength absorption bands at 14.60 and 16.80 kK (685 and 595 nm) with very different intensities 2 x 10(4) and 13.5 x 10(4)M-1 cm-1. The spectrum of the dimers in aqueous solution is in agreement with theoretical considerations of Förster (1946) and Levinson et al. (1957). It agrees with an antiparallel orientation of the molecules in the dimers. It may be that dimers bound to a substrate in the cell have another geometry than dimers in solution. In this case the weak long wavelength absorption of the dimers can increase.
天青B是最重要的罗曼诺夫斯基染料。它与伊红Y结合,能在细胞上产生著名的罗曼诺夫斯基-吉姆萨染色模式。通常市售的天青B污染严重。我们制备了一份分析纯且无有色杂质的天青B - BF4样品。该物质用于重新测定乙醇溶液中单体天青B的摩尔消光系数ε(v)M。在v = 15.61 kK(λ = 641 nm)的长波长吸收最大值处,吸光率为ε(15.61)M = (9.40 ± 0.15)×10(4)M-1 cm-1。该消光系数可用于染料样品的标准化。在水溶液中,天青B随着浓度增加会形成二聚体甚至更高的聚合物。二聚体的解离常数K = 2.2×10(-4)M(293 K),通过使用迭代程序,根据光谱的浓度依赖性计算出了水中纯单体和二聚体的吸收光谱。单体在15.47 kK(646 nm)处的摩尔消光系数为ε(15.47)M = 7.4×10(4)M-1 cm-1。二聚体在14.60和16.80 kK(685和595 nm)处有两个长波长吸收带,强度差异很大,分别为2×10(4)和13.5×10(4)M-1 cm-1。水溶液中二聚体的光谱与福斯特(1946年)和莱文森等人(1957年)的理论考虑一致。它与二聚体中分子的反平行取向相符。可能与细胞中底物结合的二聚体具有与溶液中二聚体不同的几何结构。在这种情况下,二聚体较弱的长波长吸收可能会增加。