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Dive into the research topics where Shigeki Owada is active.

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Featured researches published by Shigeki Owada.


Science | 2016

A three-dimensional movie of structural changes in bacteriorhodopsin

Eriko Nango; Antoine Royant; Minoru Kubo; Takanori Nakane; Cecilia Wickstrand; Tetsunari Kimura; Tomoyuki Tanaka; Kensuke Tono; Changyong Song; Rie Tanaka; Toshi Arima; Ayumi Yamashita; Jun Kobayashi; Toshiaki Hosaka; Eiichi Mizohata; Przemyslaw Nogly; Michihiro Sugahara; Daewoong Nam; Takashi Nomura; Tatsuro Shimamura; Dohyun Im; Takaaki Fujiwara; Yasuaki Yamanaka; Byeonghyun Jeon; Tomohiro Nishizawa; Kazumasa Oda; Masahiro Fukuda; Rebecka Andersson; Petra Båth; Robert Dods

Snapshots of bacteriorhodopsin Bacteriorhodopsin is a membrane protein that harvests the energy content from light to transport protons out of the cell against a transmembrane potential. Nango et al. used timeresolved serial femtosecond crystallography at an x-ray free electron laser to provide 13 structural snapshots of the conformational changes that occur in the nanoseconds to milliseconds after photoactivation. These changes begin at the active site, propagate toward the extracellular side of the protein, and mediate internal protonation exchanges that achieve proton transport. Science, this issue p. 1552 Time-resolved serial crystallography using an x-ray free electron laser reveals structural changes in bacteriorhodopsin. Bacteriorhodopsin (bR) is a light-driven proton pump and a model membrane transport protein. We used time-resolved serial femtosecond crystallography at an x-ray free electron laser to visualize conformational changes in bR from nanoseconds to milliseconds following photoactivation. An initially twisted retinal chromophore displaces a conserved tryptophan residue of transmembrane helix F on the cytoplasmic side of the protein while dislodging a key water molecule on the extracellular side. The resulting cascade of structural changes throughout the protein shows how motions are choreographed as bR transports protons uphill against a transmembrane concentration gradient.


Optics Express | 2011

Extreme ultraviolet free electron laser seeded with high-order harmonic of Ti:sapphire laser

Tadashi Togashi; Eiji J. Takahashi; Katsumi Midorikawa; Makoto Aoyama; Koichi Yamakawa; Takahiro Sato; Atsushi Iwasaki; Shigeki Owada; Tomoya Okino; Kaoru Yamanouchi; Fumihiko Kannari; Akira Yagishita; Hidetoshi Nakano; Marie E. Couprie; Kenji Fukami; Takaki Hatsui; Toru Hara; Takashi Kameshima; Hideo Kitamura; Noritaka Kumagai; Shinichi Matsubara; Mitsuru Nagasono; Haruhiko Ohashi; Takashi Ohshima; Yuji Otake; Tsumoru Shintake; Kenji Tamasaku; Hitoshi Tanaka; Takashi Tanaka; Kazuaki Togawa

The 13th harmonic of a Ti:sapphire (Ti:S) laser in the plateau region was injected as a seeding source to a 250-MeV free-electron-laser (FEL) amplifier. When the amplification conditions were fulfilled, strong enhancement of the radiation intensity by a factor of 650 was observed. The random and uncontrollable spikes, which appeared in the spectra of the Self-Amplified Spontaneous Emission (SASE) based FEL radiation without the seeding source, were found to be suppressed drastically to form to a narrow-band, single peak profile at 61.2 nm. The properties of the seeded FEL radiation were well reproduced by numerical simulations. We discuss the future precept of the seeded FEL scheme to the shorter wavelength region.


Nature Materials | 2016

Ultrafast energy- and momentum-resolved dynamics of magnetic correlations in the photo-doped Mott insulator Sr2IrO4

M. P. M. Dean; Yue Cao; X. Liu; Simon Wall; Diling Zhu; Roman Mankowsky; V. Thampy; X. M. Chen; J. G. Vale; D. Casa; Jungho Kim; Ayman Said; P. Juhas; Roberto Alonso-Mori; James M. Glownia; Marcin Sikorski; Sanghoon Song; M. Kozina; Henrik T. Lemke; L. Patthey; Shigeki Owada; Tetsuo Katayama; Makina Yabashi; Yoshikazu Tanaka; Tadashi Togashi; Jian Liu; C. Rayan Serrao; B. J. Kim; L. Huber; C. L. Chang

Measuring how the magnetic correlations evolve in doped Mott insulators has greatly improved our understanding of the pseudogap, non-Fermi liquids and high-temperature superconductivity. Recently, photo-excitation has been used to induce similarly exotic states transiently. However, the lack of available probes of magnetic correlations in the time domain hinders our understanding of these photo-induced states and how they could be controlled. Here, we implement magnetic resonant inelastic X-ray scattering at a free-electron laser to directly determine the magnetic dynamics after photo-doping the Mott insulator Sr2IrO4. We find that the non-equilibrium state, 2 ps after the excitation, exhibits strongly suppressed long-range magnetic order, but hosts photo-carriers that induce strong, non-thermal magnetic correlations. These two-dimensional (2D) in-plane Néel correlations recover within a few picoseconds, whereas the three-dimensional (3D) long-range magnetic order restores on a fluence-dependent timescale of a few hundred picoseconds. The marked difference in these two timescales implies that the dimensionality of magnetic correlations is vital for our understanding of ultrafast magnetic dynamics.


Optics Express | 2014

High-precision x-ray FEL pulse arrival time measurements at SACLA by a THz streak camera with Xe clusters

Pavle Juranić; A. Stepanov; Rasmus Ischebeck; V. Schlott; Claude Pradervand; L. Patthey; M. Radović; Ishkhan Gorgisyan; Leonid Rivkin; Christoph P. Hauri; B. Monoszlai; R. Ivanov; P. Peier; J. Liu; Tadashi Togashi; Shigeki Owada; Kanade Ogawa; Tetsuo Katayama; Makina Yabashi; Rafael Abela

The accurate measurement of the arrival time of a hard X-ray free electron laser (FEL) pulse with respect to a laser is of utmost importance for pump-probe experiments proposed or carried out at FEL facilities around the world. This manuscript presents the latest device to meet this challenge, a THz streak camera using Xe gas clusters, capable of pulse arrival time measurements with an estimated accuracy of several femtoseconds. An experiment performed at SACLA demonstrates the performance of the device at photon energies between 5 and 10 keV with variable photon beam parameters.


Structural Dynamics | 2016

A beam branching method for timing and spectral characterization of hard X-ray free-electron lasers

Tetsuo Katayama; Shigeki Owada; Tadashi Togashi; Kanade Ogawa; Petri Karvinen; Ismo Vartiainen; Anni Eronen; Christian David; Takahiro Sato; Kyo Nakajima; Yasumasa Joti; Hirokatsu Yumoto; Haruhiko Ohashi; Makina Yabashi

We report a method for achieving advanced photon diagnostics of x-ray free-electron lasers (XFELs) under a quasi-noninvasive condition by using a beam-splitting scheme. Here, we used a transmission grating to generate multiple branches of x-ray beams. One of the two primary diffracted branches (+1st-order) is utilized for spectral measurement in a dispersive scheme, while the other (−1st-order) is dedicated for arrival timing diagnostics between the XFEL and the optical laser pulses. The transmitted x-ray beam (0th-order) is guided to an experimental station. To confirm the validity of this timing-monitoring scheme, we measured the correlation between the arrival timings of the −1st and 0th branches. The observed error was as small as 7.0 fs in root-mean-square. Our result showed the applicability of the beam branching scheme to advanced photon diagnostics, which will further enhance experimental capabilities of XFEL.


Proceedings of the National Academy of Sciences of the United States of America | 2016

Observation of femtosecond X-ray interactions with matter using an X-ray–X-ray pump–probe scheme

Ichiro Inoue; Yuichi Inubushi; Takahiro Sato; Kensuke Tono; Tetsuo Katayama; Takashi Kameshima; Kanade Ogawa; Tadashi Togashi; Shigeki Owada; Yoshiyuki Amemiya; Takashi Tanaka; Toru Hara; Makina Yabashi

Significance Understanding ultraintense light–matter interactions is an intriguing subject from viewpoints of basic science and practical applications. For the X-ray region, such research fields have opened up with the emergence of X-ray free-electron lasers (XFELs). By using an X-ray–X-ray pump–probe scheme, we firstly measured atomic response to XFEL light with femtosecond–ångstrom time–space resolutions. It was found that the atomic position is freezing until 20 fs after the XFEL irradiation, which supports the feasibility of damageless structural determinations with ultraintense XFEL pulses. The pump–probe scheme demonstrated here is an effective way to capture X-ray–matter interactions, and would contribute to verify and improve theory of X-ray interactions with matter, and stimulate advanced XFEL applications. Resolution in the X-ray structure determination of noncrystalline samples has been limited to several tens of nanometers, because deep X-ray irradiation required for enhanced resolution causes radiation damage to samples. However, theoretical studies predict that the femtosecond (fs) durations of X-ray free-electron laser (XFEL) pulses make it possible to record scattering signals before the initiation of X-ray damage processes; thus, an ultraintense X-ray beam can be used beyond the conventional limit of radiation dose. Here, we verify this scenario by directly observing femtosecond X-ray damage processes in diamond irradiated with extraordinarily intense (∼1019 W/cm2) XFEL pulses. An X-ray pump–probe diffraction scheme was developed in this study; tightly focused double–5-fs XFEL pulses with time separations ranging from sub-fs to 80 fs were used to excite (i.e., pump) the diamond and characterize (i.e., probe) the temporal changes of the crystalline structures through Bragg reflection. It was found that the pump and probe diffraction intensities remain almost constant for shorter time separations of the double pulse, whereas the probe diffraction intensities decreased after 20 fs following pump pulse irradiation due to the X-ray–induced atomic displacement. This result indicates that sub-10-fs XFEL pulses enable conductions of damageless structural determinations and supports the validity of the theoretical predictions of ultraintense X-ray–matter interactions. The X-ray pump–probe scheme demonstrated here would be effective for understanding ultraintense X-ray–matter interactions, which will greatly stimulate advanced XFEL applications, such as atomic structure determination of a single molecule and generation of exotic matters with high energy densities.


Structural Dynamics | 2015

Ultraviolet photochemical reaction of [Fe(III)(C2O4)3]3− in aqueous solutions studied by femtosecond time-resolved X-ray absorption spectroscopy using an X-ray free electron laser

Yoshihiro Ogi; Yuki Obara; Tetsuo Katayama; Y.-I. Suzuki; S. Y. Liu; N. C.-M. Bartlett; Naoya Kurahashi; Shutaro Karashima; Tadashi Togashi; Yuichi Inubushi; K. Ogawa; Shigeki Owada; Martina Rubešová; Makina Yabashi; Kazuhiko Misawa; Petr Slavíček; Toshinori Suzuki

Time-resolved X-ray absorption spectroscopy was performed for aqueous ammonium iron(III) oxalate trihydrate solutions using an X-ray free electron laser and a synchronized ultraviolet laser. The spectral and time resolutions of the experiment were 1.3 eV and 200 fs, respectively. A femtosecond 268 nm pulse was employed to excite [Fe(III)(C2O4)3]3− in solution from the high-spin ground electronic state to ligand-to-metal charge transfer state(s), and the subsequent dynamics were studied by observing the time-evolution of the X-ray absorption spectrum near the Fe K-edge. Upon 268 nm photoexcitation, the Fe K-edge underwent a red-shift by more than 4 eV within 140 fs; however, the magnitude of the redshift subsequently diminished within 3 ps. The Fe K-edge of the photoproduct remained lower in energy than that of [Fe(III)(C2O4)3]3−. The observed red-shift of the Fe K-edge and the spectral feature of the product indicate that Fe(III) is upon excitation immediately photoreduced to Fe(II), followed by ligand dissociation from Fe(II). Based on a comparison of the X-ray absorption spectra with density functional theory calculations, we propose that the dissociation proceeds in two steps, forming first [(CO2•)Fe(II)(C2O4)2]3− and subsequently [Fe(II)(C2O4)2]2−.


Optics Express | 2017

THz streak camera method for synchronous arrival time measurement of two-color hard X-ray FEL pulses

Ishkhan Gorgisyan; Rasmus Ischebeck; Christian Erny; A. Dax; L. Patthey; Claude Pradervand; Leonardo Sala; Christopher J. Milne; Henrik T. Lemke; Christoph P. Hauri; Tetsuo Katayama; Shigeki Owada; Makina Yabashi; Tadashi Togashi; Rafael Abela; Leonid Rivkin; Pavle Juranić

The two-color operation of free electron laser (FEL) facilities allows the delivery of two FEL pulses with different energies, which opens new possibilities for user experiments. Measuring the arrival time of both FEL pulses relative to the external experimental laser and to each other improves the temporal resolution of the experiments using the two-color FEL beam and helps to monitor the performance of the machine itself. This work reports on the first simultaneous measurement of the arrival times of two hard X-ray FEL pulses with the THz streak camera. Measuring the arrival time of the two FEL pulses, the relative delay between them was calculated and compared to the set values. Furthermore, we present the first comparison of the THz streak camera method to the method of FEL induced transient transmission. The results indicate a good agreement between the two methods.


Science Advances | 2017

A nanosecond time-resolved XFEL analysis of structural changes associated with CO release from cytochrome C oxidase

Atsuhiro Shimada; Minoru Kubo; Seiki Baba; Keitaro Yamashita; Kunio Hirata; Go Ueno; Takashi Nomura; Tetsunari Kimura; Kyoko Shinzawa-Itoh; Junpei Baba; Keita Hatano; Yuki Eto; Akari Miyamoto; Hironori Murakami; Takashi Kumasaka; Shigeki Owada; Kensuke Tono; Makina Yabashi; Yoshihiro Yamaguchi; Sachiko Yanagisawa; Miyuki Sakaguchi; Takashi Ogura; Ryo Komiya; Jiwang Yan; Eiki Yamashita; Masaki Yamamoto; Hideo Ago; Shinya Yoshikawa; Tomitake Tsukihara

XFEL and IR analyses suggest that O2 bound at CuB blocks proton backflow for unidirectional H+ transport by water channel closure. Bovine cytochrome c oxidase (CcO), a 420-kDa membrane protein, pumps protons using electrostatic repulsion between protons transferred through a water channel and net positive charges created by oxidation of heme a (Fea) for reduction of O2 at heme a3 (Fea3). For this process to function properly, timing is essential: The channel must be closed after collection of the protons to be pumped and before Fea oxidation. If the channel were to remain open, spontaneous backflow of the collected protons would occur. For elucidation of the channel closure mechanism, the opening of the channel, which occurs upon release of CO from CcO, is investigated by newly developed time-resolved x-ray free-electron laser and infrared techniques with nanosecond time resolution. The opening process indicates that CuB senses completion of proton collection and binds O2 before binding to Fea3 to close the water channel using a conformational relay system, which includes CuB, heme a3, and a transmembrane helix, to block backflow of the collected protons.


Journal of Synchrotron Radiation | 2018

A soft X-ray free-electron laser beamline at SACLA: the light source, photon beamline and experimental station

Shigeki Owada; Kazuaki Togawa; Takahiro Inagaki; Toru Hara; Takashi Tanaka; Yasumasa Joti; Takahisa Koyama; Kyo Nakajima; Haruhiko Ohashi; Y. Senba; Tadashi Togashi; Kensuke Tono; Mitsuhiro Yamaga; Hirokatsu Yumoto; Makina Yabashi; Hitoshi Tanaka; Tetsuya Ishikawa

The status of a soft X-ray free-electron laser beamline at SACLA is reported.

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Kanade Ogawa

Japan Atomic Energy Agency

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