Cehelnik E D, Mielenz K D, Velapoldi R A
Institute for Materials Research, National Bureau of Standards, Washington, D.C. 20234.
J Res Natl Bur Stand A Phys Chem. 1975 Jan-Feb;79A(1):1-15. doi: 10.6028/jres.079A.001.
Polarization effects on fluorescence measurements are a function of four independent variables. The first is , the polarization ratio of the exciting light which reaches the sample. The second is , the emission anisotropy of the sample, which is the polarization "response" of the sample to plane polarized exciting light. The third is , the polarization ratio of the emission detection system, which is the ratio of the sensitivities of the detection system to vertically and horizontally polarized light. The fourth is α the viewing angle, which is the angle bet ween the direction of the propagation of the exciting light and the direction from which the emission is being detected. The intensity and the degree of polarization of the fluorescence emission that the sample exhibits are functions of , , and , while the actual readings obtained with a typical spectrofluorimeter are functions of all four variables, , , , and . A theoretical analysis is made taking all these factors into account, and proper mathematical models are developed for the different modes of operation in which a fluorimeter can be used. These are verified experimentally with data obtained for a sample which has a high degree of emission anisotropy (Nile Blue A Perchlorate in glycerol). A recently designed goniospectrofluorimeter was used. Calibration procedures are developed and recommendations are made for modes of operation and fluorescence standards.
荧光测量中的偏振效应是四个独立变量的函数。第一个变量是 ,即到达样品的激发光的偏振比。第二个变量是 ,即样品的发射各向异性,它是样品对平面偏振激发光的偏振“响应”。第三个变量是 ,即发射检测系统的偏振比,它是检测系统对垂直偏振光和水平偏振光的灵敏度之比。第四个变量是α,即视角,它是激发光传播方向与发射光检测方向之间的夹角。样品所呈现的荧光发射的强度和偏振度是 、 和 的函数,而用典型的荧光分光光度计获得的实际读数则是所有四个变量 、 、 和 的函数。考虑到所有这些因素进行了理论分析,并针对荧光计可以使用的不同操作模式建立了适当的数学模型。使用具有高发射各向异性的样品(甘油中的高氯酸盐尼罗蓝A)获得的数据对这些模型进行了实验验证。使用了最近设计的测角荧光分光光度计。制定了校准程序,并对操作模式和荧光标准提出了建议。