Effects of x-ray free-electron laser pulse intensity on the Mn K β 1,3 x-ray emission spectrum in photosystem II-A case study for metalloprotein crystals and solutions.

IF 2.3 2区 物理与天体物理 Q3 CHEMISTRY, PHYSICAL Structural Dynamics-Us Pub Date : 2021-11-22 eCollection Date: 2021-11-01 DOI:10.1063/4.0000130
Thomas Fransson, Roberto Alonso-Mori, Ruchira Chatterjee, Mun Hon Cheah, Mohamed Ibrahim, Rana Hussein, Miao Zhang, Franklin Fuller, Sheraz Gul, In-Sik Kim, Philipp S Simon, Isabel Bogacz, Hiroki Makita, Casper de Lichtenberg, Sanghoon Song, Alexander Batyuk, Dimosthenis Sokaras, Ramzi Massad, Margaret Doyle, Alexander Britz, Clemens Weninger, Athina Zouni, Johannes Messinger, Vittal K Yachandra, Junko Yano, Jan Kern, Uwe Bergmann
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Abstract

In the last ten years, x-ray free-electron lasers (XFELs) have been successfully employed to characterize metalloproteins at room temperature using various techniques including x-ray diffraction, scattering, and spectroscopy. The approach has been to outrun the radiation damage by using femtosecond (fs) x-ray pulses. An example of an important and damage sensitive active metal center is the Mn4CaO5 cluster in photosystem II (PS II), the catalytic site of photosynthetic water oxidation. The combination of serial femtosecond x-ray crystallography and Kβ x-ray emission spectroscopy (XES) has proven to be a powerful multimodal approach for simultaneously probing the overall protein structure and the electronic state of the Mn4CaO5 cluster throughout the catalytic (Kok) cycle. As the observed spectral changes in the Mn4CaO5 cluster are very subtle, it is critical to consider the potential effects of the intense XFEL pulses on the Kβ XES signal. We report here a systematic study of the effects of XFEL peak power, beam focus, and dose on the Mn Kβ1,3 XES spectra in PS II over a wide range of pulse parameters collected over seven different experimental runs using both microcrystal and solution PS II samples. Our findings show that for beam intensities ranging from ∼5 × 1015 to 5 × 1017 W/cm2 at a pulse length of ∼35 fs, the spectral effects are small compared to those observed between S-states in the Kok cycle. Our results provide a benchmark for other XFEL-based XES studies on metalloproteins, confirming the viability of this approach.

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X 射线自由电子激光脉冲强度对光系统 II 中 Mn K β 1,3 X 射线发射光谱的影响--金属蛋白晶体和溶液的案例研究。
在过去十年中,X 射线自由电子激光器(XFEL)已被成功地用于在室温下使用各种技术(包括 X 射线衍射、散射和光谱学)表征金属蛋白。其方法是利用飞秒 (fs) X 射线脉冲来超越辐射损伤。光系统 II(PS II)中的 Mn4CaO5 簇是一个重要的、对损伤敏感的活性金属中心,它是光合作用水氧化的催化场所。串行飞秒 X 射线晶体学和 Kβ X 射线发射光谱(XES)的结合被证明是一种强大的多模式方法,可同时探测整个蛋白质结构和 Mn4CaO5 簇在整个催化(Kok)循环中的电子状态。由于在 Mn4CaO5 团簇中观察到的光谱变化非常微妙,因此考虑强 XFEL 脉冲对 Kβ XES 信号的潜在影响至关重要。我们在此报告了一项系统性研究,研究了 XFEL 峰值功率、光束聚焦和剂量对 PS II 中 Mn Kβ1,3 XES 光谱的影响,该研究使用微晶和溶液 PS II 样品,在七个不同的实验运行中收集了广泛的脉冲参数。我们的研究结果表明,在脉冲长度为 ∼35 fs 时,光束强度范围为 ∼5 × 1015 至 5 × 1017 W/cm2,与在 Kok 循环中的 S 态之间观察到的光谱效应相比,光谱效应很小。我们的研究结果为其他基于 XFEL 的金属蛋白 XES 研究提供了基准,证实了这种方法的可行性。
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来源期刊
Structural Dynamics-Us
Structural Dynamics-Us CHEMISTRY, PHYSICALPHYSICS, ATOMIC, MOLECU-PHYSICS, ATOMIC, MOLECULAR & CHEMICAL
CiteScore
5.50
自引率
3.60%
发文量
24
审稿时长
16 weeks
期刊介绍: Structural Dynamics focuses on the recent developments in experimental and theoretical methods and techniques that allow a visualization of the electronic and geometric structural changes in real time of chemical, biological, and condensed-matter systems. The community of scientists and engineers working on structural dynamics in such diverse systems often use similar instrumentation and methods. The journal welcomes articles dealing with fundamental problems of electronic and structural dynamics that are tackled by new methods, such as: Time-resolved X-ray and electron diffraction and scattering, Coherent diffractive imaging, Time-resolved X-ray spectroscopies (absorption, emission, resonant inelastic scattering, etc.), Time-resolved electron energy loss spectroscopy (EELS) and electron microscopy, Time-resolved photoelectron spectroscopies (UPS, XPS, ARPES, etc.), Multidimensional spectroscopies in the infrared, the visible and the ultraviolet, Nonlinear spectroscopies in the VUV, the soft and the hard X-ray domains, Theory and computational methods and algorithms for the analysis and description of structuraldynamics and their associated experimental signals. These new methods are enabled by new instrumentation, such as: X-ray free electron lasers, which provide flux, coherence, and time resolution, New sources of ultrashort electron pulses, New sources of ultrashort vacuum ultraviolet (VUV) to hard X-ray pulses, such as high-harmonic generation (HHG) sources or plasma-based sources, New sources of ultrashort infrared and terahertz (THz) radiation, New detectors for X-rays and electrons, New sample handling and delivery schemes, New computational capabilities.
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