Heinz Walz GmbH, Eichenring 6, 91090, Effeltrich, Germany.
Photosynth Res. 2021 Mar;147(3):345-358. doi: 10.1007/s11120-021-00821-7. Epub 2021 Feb 2.
PAM fluorescence of leaves of cherry laurel (Prunus laurocerasus L.) was measured simultaneously in the spectral range below 700 nm (sw) and above 700 nm (lw). A high-sensitivity photodiode was employed to measure the low intensities of sw fluorescence. Photosystem II (PSII) performance was analyzed by the saturation pulse method during a light response curve with subsequent dark phase. The sw fluorescence was more variable, resulting in higher PSII photochemical yields compared to lw fluorescence. The variations between sw and lw data were explained by different levels of photosystem I (PSI) fluorescence: the contribution of PSI fluorescence to minimum fluorescence (F) was calculated to be 14% at sw wavelengths and 45% at lw wavelengths. With the results obtained, the validity of an earlier method for the quantification of PSI fluorescence (Genty et al. in Photosynth Res 26:133-139, 1990, https://doi.org/10.1007/BF00047085 ) was reconsidered. After subtracting PSI fluorescence from all fluorescence levels, the maximum PSII photochemical yield (F/F) in the sw range was 0.862 and it was 0.883 in the lw range. The lower F/F at sw wavelengths was suggested to arise from inactive PSII reaction centers in the outermost leaf layers. Polyphasic fluorescence transients (OJIP or OIIP kinetics) were recorded simultaneously at sw and lw wavelengths: the slowest phase of the kinetics (IP or IP) corresponded to 11% and 13% of total variable sw and lw fluorescence, respectively. The idea that this difference is due to variable PSI fluorescence is critically discussed. Potential future applications of simultaneously recording fluorescence in two spectral windows include studies of PSI non-photochemical quenching and state I-state II transitions, as well as measuring the fluorescence from pH-sensitive dyes simultaneously with chlorophyll fluorescence.
樱桃李(Prunus laurocerasus L.)叶片的 PAM 荧光在 700nm 以下(sw)和 700nm 以上(lw)的光谱范围内同时测量。高灵敏度光电二极管用于测量 sw 荧光的低强度。在光响应曲线期间,通过饱和脉冲法分析光系统 II(PSII)性能,随后进行暗相。与 lw 荧光相比,sw 荧光变化更大,导致 PSII 光化学产率更高。sw 和 lw 数据之间的差异可以通过不同水平的光系统 I(PSI)荧光来解释:PSI 荧光对最小荧光(F)的贡献在 sw 波长下计算为 14%,在 lw 波长下计算为 45%。根据所得到的结果,重新考虑了一种早期用于量化 PSI 荧光的方法的有效性(Genty 等人,在 Photosynth Res 26:133-139,1990 年,https://doi.org/10.1007/BF00047085)。从所有荧光水平中减去 PSI 荧光后,sw 范围内的最大 PSII 光化学产率(F/F)为 0.862,lw 范围内为 0.883。sw 波长下较低的 F/F 被认为是由于最外层叶片层中无活性的 PSII 反应中心。在 sw 和 lw 波长下同时记录多相荧光瞬变(OJIP 或 OIIP 动力学):动力学的最慢相(IP 或 IP)分别对应于总可变 sw 和 lw 荧光的 11%和 13%。批判性地讨论了这种差异是由于可变 PSI 荧光的观点。同时在两个光谱窗口记录荧光的潜在未来应用包括 PSI 非光化学猝灭和状态 I-状态 II 转变的研究,以及同时测量 pH 敏感染料的荧光和叶绿素荧光。