Koulougliotis D, Schweitzer R H, Brudvig G W
Department of Chemistry, Yale University, New Haven, Connecticut 06520-8107, USA.
Biochemistry. 1997 Aug 12;36(32):9735-46. doi: 10.1021/bi970326t.
The spin-lattice relaxation enhancement of the dark-stable tyrosine radical, YD., by the S2 state of the O2-evolving complex (OEC) of photosystem II (PSII) has been measured by using saturation-recovery EPR spectroscopy. Two forms of the S2 state have been compared: the multiline EPR signal species in untreated PSII and the altered multiline EPR signal species in NH3-treated PSII. Previous work has shown that the non-single-exponential spin-lattice relaxation kinetics of YD. in S2-state PSII result from a dipole-dipole interaction with the Mn4 cluster of the OEC. By taking into account the temperature variation of the effective magnetic moment of the S2-state multiline EPR signal form of the OEC, we provide a quantitative analysis of its temperature-dependent enhancement of the spin-lattice relaxation of YD.. Different spin states of the Mn4 cluster in the S2 state are responsible for the effect at different temperature regimes: for T </= 10 K, it is the ground spin state (S = 1/2); for T >/= 30 K, it is the first excited spin state; and at intermediate temperatures, the contributions of the two spin states are comparable. The relaxation enhancement of YD. is equivalent for both forms of the S2-state multiline EPR signal examined, indicating that the magnetic properties of the Mn4 cluster are very similar in the S2 state for both untreated and NH3-treated PSII. EPR progressive microwave-power saturation has also been used to assess the spin-lattice relaxation properties of the Mn4 cluster giving the altered S2-state multiline EPR signal in the NH3 derivative of PSII. The Orbach mechanism is shown to provide the dominant relaxation pathway; the energy difference between the ground and first excited spin states is estimated to be 30 +/- 2 cm-1, which is very similar to the value found for the S2-state multiline EPR signal species in untreated PSII. Below 4 K, the effectiveness of the S2-state multiline EPR signal species as a spin relaxation enhancer of YD. drops dramatically. This is interpreted to occur because of temperature-dependent 55Mn nuclear spin-lattice relaxation which causes averaging of the effective Larmor frequency of the S2-state multiline EPR signal species during the time scale for spin-lattice relaxation of YD.; because the line shape of the S2-state multiline EPR signal is dominated by isotropic 55Mn nuclear hyperfine splittings, such nuclear relaxation processes allow frequencies in near resonance with that of YD. to be accessed, thereby producing a greater relaxation enhancement. By using a dipolar model that includes the line shapes of both the YD. and S2-state multiline EPR signals, the spin-lattice relaxation enhancement of YD. is analyzed to obtain a lower limit of 22 A for the distance between YD. and the OEC. Together with recent studies showing a close proximity of the Mn4 cluster to YZ., these results provide further support for an asymmetric location of the Mn4 cluster with respect to the two redox-active tyrosines in PSII.
通过饱和恢复电子顺磁共振光谱法,测量了光系统II(PSII)的放氧复合体(OEC)的S2态对暗稳定酪氨酸自由基YD.的自旋 - 晶格弛豫增强作用。比较了S2态的两种形式:未处理的PSII中的多线电子顺磁共振信号种类和经NH3处理的PSII中改变后的多线电子顺磁共振信号种类。先前的研究表明,YD.在S2态PSII中的非单指数自旋 - 晶格弛豫动力学是由与OEC的Mn4簇的偶极 - 偶极相互作用引起的。通过考虑OEC的S2态多线电子顺磁共振信号形式的有效磁矩的温度变化,我们对其温度依赖性的YD.自旋 - 晶格弛豫增强进行了定量分析。S2态中Mn4簇的不同自旋态在不同温度范围内起作用:对于T≤10K,是基态自旋态(S = 1/2);对于T≥30K,是第一激发自旋态;在中间温度下,两种自旋态的贡献相当。对于所研究的S2态多线电子顺磁共振信号的两种形式,YD.的弛豫增强是等效的,这表明在未处理和经NH3处理的PSII的S2态中,Mn4簇的磁性非常相似。电子顺磁共振渐进微波功率饱和也已用于评估在PSII的NH3衍生物中给出改变后的S2态多线电子顺磁共振信号的Mn4簇的自旋 - 晶格弛豫特性。结果表明,奥尔巴赫机制提供了主要的弛豫途径;基态和第一激发自旋态之间的能量差估计为30±2cm-1,这与在未处理的PSII中S2态多线电子顺磁共振信号种类中发现的值非常相似。在4K以下,S2态多线电子顺磁共振信号种类作为YD.的自旋弛豫增强剂的有效性急剧下降。这被解释为是由于温度依赖性的55Mn核自旋 - 晶格弛豫,它导致在YD.的自旋 - 晶格弛豫时间尺度内S2态多线电子顺磁共振信号种类的有效拉莫尔频率平均化;因为S2态多线电子顺磁共振信号的线形由各向同性的55Mn核超精细分裂主导,这种核弛豫过程允许接近YD.频率的频率被访问,从而产生更大的弛豫增强。通过使用一个包括YD.和S2态多线电子顺磁共振信号线形的偶极模型,分析了YD.的自旋 - 晶格弛豫增强,以获得YD.与OEC之间距离的下限为22Å。连同最近显示Mn4簇与YZ.紧密接近的研究,这些结果为Mn4簇相对于PSII中两个氧化还原活性酪氨酸的不对称位置提供了进一步的支持。