Institute of Life Science, National Tsing Hua University, 30043, Hsin-Chu, Taiwan, Republic of China.
Photosynth Res. 1991 Feb;27(2):143-50. doi: 10.1007/BF00033253.
In order to characterize the photosystem II (PS II) centers which are inactive in plastoquinone reduction, the initial variable fluorescence rise from the non-variable fluorescence level Fo to an intermediate plateau level Fi has been studied. We find that the initial fluorescence rise is a monophasic exponential function of time. Its rate constant is similar to the initial rate of the fastest phase (α-phase) of the fluorescence induction curve from DCMU-poisoned chloroplasts. In addition, the initial fluorescence rise and the α-phase have the following common properties: their rate constants vary linearly with excitation light intensity and their fluorescence yields are lowered by removal of Mg(++) from the suspension medium. We suggest that the inactive PS II centers, which give rise to the fluorescence rise from Fo to Fi, belong to the α-type PS II centers. However, since these inactive centers do not display sigmoidicity in fluorescence, they thus do not allow energy transfer between PS II units like PS IIα.
为了描述在去镁叶绿素(DCMU)抑制条件下不参与质体醌还原的光系统 II(PS II)中心的特征,我们研究了初始可变荧光从不变荧光 Fo 上升到中间平台水平 Fi 的过程。我们发现初始荧光上升是时间的单指数函数。其速率常数与 DCMU 抑制的叶绿体荧光诱导曲线最快相(α相)的初始速率相似。此外,初始荧光上升和α相具有以下共同性质:它们的速率常数与激发光强度呈线性变化,而它们的荧光产率则因悬浮介质中 Mg(++)的去除而降低。我们认为,引起 Fo 到 Fi 荧光上升的失活 PS II 中心属于α型 PS II 中心。然而,由于这些失活中心在荧光中不显示出“S”形,因此它们不像 PS IIα那样允许 PS II 单元之间的能量转移。