Miyake Chikahiro, Shinzaki Yuki, Miyata Momoko, Tomizawa Ken-ichi
Research Institute of Innovative Technology for the Earth (RITE), 9-2 Kizugawadai, Kizu-cho, Soraku-gun, Kyoto, 619-0292 Japan.
Plant Cell Physiol. 2004 Oct;45(10):1426-33. doi: 10.1093/pcp/pch163.
Non-photochemical quenching (NPQ) of Chl fluorescence is a mechanism for dissipating excess photon energy and is dependent on the formation of a DeltapH across the thylakoid membranes. The role of cyclic electron flow around photosystem I (PSI) (CEF-PSI) in the formation of this DeltapH was elucidated by studying the relationships between O2-evolution rate [V(O2)], quantum yield of both PSII and PSI [Phi(PSII) and Phi(PSI)], and Chl fluorescence parameters measured simultaneously in intact leaves of tobacco plants in CO2-saturated air. Although increases in light intensity raised V(O2) and the relative electron fluxes through both PSII and PSI [Phi(PSII) x PFD and Phi(PSI) x PFD] only Phi(PSI) x PFD continued to increase after V(O2) and Phi(PSII) x PFD became light saturated. These results revealed the activity of an electron transport reaction in PSI not related to photosynthetic linear electron flow (LEF), namely CEF-PSI. NPQ of Chl fluorescence drastically increased after Phi(PSII) x PFD became light saturated and the values of NPQ correlated positively with the relative activity of CEF-PSI. At low temperatures, the light-saturation point of Phi(PSII) x PFD was lower than that of Phi(PSI) x PFD and NPQ was high. On the other hand, at high temperatures, the light-dependence curves of Phi(PSII) x PFD and Phi(PSI) x PFD corresponded completely and NPQ was not induced. These results indicate that limitation of LEF induced CEF-PSI, which, in turn, helped to dissipate excess photon energy by driving NPQ of Chl fluorescence.
叶绿素荧光的非光化学猝灭(NPQ)是一种耗散过剩光子能量的机制,它依赖于类囊体膜两侧ΔpH的形成。通过研究在CO₂饱和空气中烟草植株完整叶片中同时测量的O₂释放速率[V(O₂)]、光系统II和光系统I的量子产率[Φ(PSII)和Φ(PSI)]以及叶绿素荧光参数之间的关系,阐明了围绕光系统I(PSI)的循环电子流(CEF-PSI)在这种ΔpH形成中的作用。尽管光强增加提高了V(O₂)以及通过光系统II和光系统I的相对电子通量[Φ(PSII)×PFD和Φ(PSI)×PFD],但在V(O₂)和Φ(PSII)×PFD达到光饱和后,只有Φ(PSI)×PFD继续增加。这些结果揭示了PSI中与光合线性电子流(LEF)无关的电子传递反应的活性,即CEF-PSI。在Φ(PSII)×PFD达到光饱和后,叶绿素荧光的NPQ急剧增加,并且NPQ值与CEF-PSI的相对活性呈正相关。在低温下,Φ(PSII)×PFD的光饱和点低于Φ(PSI)×PFD的光饱和点,并且NPQ较高。另一方面,在高温下,Φ(PSII)×PFD和Φ(PSI)×PFD的光响应曲线完全对应,并且不会诱导NPQ。这些结果表明,LEF的限制诱导了CEF-PSI,而CEF-PSI反过来通过驱动叶绿素荧光的NPQ来帮助耗散过剩的光子能量。