B. Albertazzi
Osaka University
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Featured researches published by B. Albertazzi.
Science | 2014
B. Albertazzi; A. Ciardi; M. Nakatsutsumi; T. Vinci; J. Béard; R. Bonito; J. Billette; M. Borghesi; Z. Burkley; S. N. Chen; T. E. Cowan; T. Herrmannsdörfer; D. P. Higginson; F. Kroll; Sergey A. Pikuz; K. Naughton; L. Romagnani; C. Riconda; Guilhem Revet; R. Riquier; H.-P. Schlenvoigt; I. Yu. Skobelev; A. Ya. Faenov; Alexander A. Soloviev; M. Huarte-Espinosa; A. Frank; O. Portugall; H. Pépin; J. Fuchs
Although bipolar jets are seen emerging from a wide variety of astrophysical systems, the issue of their formation and morphology beyond their launching is still under study. Our scaled laboratory experiments, representative of young stellar object outflows, reveal that stable and narrow collimation of the entire flow can result from the presence of a poloidal magnetic field whose strength is consistent with observations. The laboratory plasma becomes focused with an interior cavity. This gives rise to a standing conical shock from which the jet emerges. Following simulations of the process at the full astrophysical scale, we conclude that it can also explain recently discovered x-ray emission features observed in low-density regions at the base of protostellar jets, such as the well-studied jet HH 154. A scaled-down plasma experiment shows that axial magnetic fields in young stars can shape their bipolar jet outflows. Stellar outflows replicated in miniature Astronomers observe tight bright jets beaming from the poles of many celestial objects. But what focuses them so well? Albertazzi et al. recreated a scaled-down plasma jet in a laboratory setting to match the behavior of those in young stellar objects. The experiments show that the jets are collimated by a poloidal magnetic field aligned with the same axis. A conelike shock also emerges, as the expanding plasma is abruptly confined by the magnetic field. Science, this issue p. 325
Scientific Reports | 2016
Tatiana A. Pikuz; Anatoly Ya. Faenov; Takeshi Matsuoka; Satoshi Matsuyama; Kazuto Yamauchi; Norimasa Ozaki; B. Albertazzi; Yuichi Inubushi; Makina Yabashi; Kensuke Tono; Yuya Sato; Hirokatsu Yumoto; Haruhiko Ohashi; Sergei Pikuz; A N Grum-Grzhimailo; M. Nishikino; Tetsuya Kawachi; Tetsuya Ishikawa; R. Kodama
Here, we report, that by means of direct irradiation of lithium fluoride a (LiF) crystal, in situ 3D visualization of the SACLA XFEL focused beam profile along the propagation direction is realized, including propagation inside photoluminescence solid matter. High sensitivity and large dynamic range of the LiF crystal detector allowed measurements of the intensity distribution of the beam at distances far from the best focus as well as near the best focus and evaluation of XFEL source size and beam quality factor M2. Our measurements also support the theoretical prediction that for X-ray photons with energies ~10 keV the radius of the generated photoelectron cloud within the LiF crystal reaches about 600 nm before thermalization. The proposed method has a spatial resolution ~ 0.4–2.0 μm for photons with energies 6–14 keV and potentially could be used in a single shot mode for optimization of different focusing systems developed at XFEL and synchrotron facilities.
New Journal of Physics | 2016
Nicholas Dover; C. A. J. Palmer; Matthew Streeter; H. Ahmed; B. Albertazzi; M. Borghesi; D. C. Carroll; Jean-Noël Fuchs; R. Heathcote; P. Hilz; K. F. Kakolee; S. Kar; R. Kodama; A. Kon; D. A. MacLellan; P. McKenna; S. R. Nagel; D. Neely; M. Notley; M. Nakatsutsumi; R. Prasad; G. G. Scott; M. Tampo; M. Zepf; Jörg Schreiber; Z. Najmudin
Spectrally-peaked proton beams of high charge (E-p approximate to 8 MeV, Delta E approximate to 4 MeV, N approximate to 50 nC) have been observed from the interaction of an intense laser (> 10(19) W cm(-2)) with ultrathin CH foils, as measured by spectrally-resolved full beam profiles. These beams are reproducibly generated for foil thicknesses 5-100 nm, and exhibit narrowing divergence with decreasing target thickness down to approximate to 8 degrees for 5 nm. Simulations demonstrate that the narrow energy spread feature is a result of buffered acceleration of protons. The radiation pressure at the front of the target results in asymmetric sheath fields which permeate throughout the target, causing preferential forward acceleration. Due to their higher charge-to-mass ratio, the protons outrun a carbon plasma driven in the relativistic transparency regime.
Science Advances | 2016
Toshimori Sekine; Norimasa Ozaki; Kohei Miyanishi; Yuto Asaumi; Tomoaki Kimura; B. Albertazzi; Yuya Sato; Youichi Sakawa; Takayoshi Sano; Seiji Sugita; Takafumi Matsui; R. Kodama
Shocked forsterite above 250 GPa indicates incongruent crystallization of MgO, its phase transition, and remelting. Forsterite (Mg2SiO4) is one of the major planetary materials, and its behavior under extreme conditions is important to understand the interior structure of large planets, such as super-Earths, and large-scale planetary impact events. Previous shock compression measurements of forsterite indicate that it may melt below 200 GPa, but these measurements did not go beyond 200 GPa. We report the shock response of forsterite above ~250 GPa, obtained using the laser shock wave technique. We simultaneously measured the Hugoniot and temperature of shocked forsterite and interpreted the results to suggest the following: (i) incongruent crystallization of MgO at 271 to 285 GPa, (ii) phase transition of MgO at 285 to 344 GPa, and (iii) remelting above ~470 to 500 GPa. These exothermic and endothermic reactions are seen to occur under extreme conditions of pressure and temperature. They indicate complex structural and chemical changes in the system MgO-SiO2 at extreme pressures and temperatures and will affect the way we understand the interior processes of large rocky planets as well as material transformation by impacts in the formation of planetary systems.
Science Advances | 2017
B. Albertazzi; Norimasa Ozaki; V. V. Zhakhovsky; Anatoly Ya. Faenov; H. Habara; Marion Harmand; N. J. Hartley; Denis Ilnitsky; N. A. Inogamov; Yuichi Inubushi; Tetsuya Ishikawa; Tetsuo Katayama; Takahisa Koyama; M. Koenig; Andrew Krygier; Takeshi Matsuoka; Satoshi Matsuyama; E. E. McBride; K. P. Migdal; G. Morard; Haruhiko Ohashi; Takuo Okuchi; Tatiana A. Pikuz; Narangoo Purevjav; Osami Sakata; Yasuhisa Sano; Tomoko Sato; Toshimori Sekine; Yusuke Seto; Kenjiro Takahashi
The dynamic fracture of tantalum is observed at the atomic scale using an x-ray monitoring technique at the SACLA XFEL facility. The understanding of fracture phenomena of a material at extremely high strain rates is a key issue for a wide variety of scientific research ranging from applied science and technological developments to fundamental science such as laser-matter interaction and geology. Despite its interest, its study relies on a fine multiscale description, in between the atomic scale and macroscopic processes, so far only achievable by large-scale atomic simulations. Direct ultrafast real-time monitoring of dynamic fracture (spallation) at the atomic lattice scale with picosecond time resolution was beyond the reach of experimental techniques. We show that the coupling between a high-power optical laser pump pulse and a femtosecond x-ray probe pulse generated by an x-ray free electron laser allows detection of the lattice dynamics in a tantalum foil at an ultrahigh strain rate of ε. ~2 × 108 to 3.5 × 108 s−1. A maximal density drop of 8 to 10%, associated with the onset of spallation at a spall strength of ~17 GPa, was directly measured using x-ray diffraction. The experimental results of density evolution agree well with large-scale atomistic simulations of shock wave propagation and fracture of the sample. Our experimental technique opens a new pathway to the investigation of ultrahigh strain-rate phenomena in materials at the atomic scale, including high-speed crack dynamics and stress-induced solid-solid phase transitions.
Physics of Plasmas | 2017
M. Koenig; Th. Michel; R. Yurchak; C. Michaut; B. Albertazzi; S. Laffite; E. Falize; L. Van Box Som; Youichi Sakawa; Tomokazu Sano; Y. Hara; T. Morita; Yasuhiro Kuramitsu; P. Barroso; A. Pelka; G. Gregori; R. Kodama; Norio Ozaki; D. Q. Lamb; P. Tzeferacos
In this paper, we present the recent results obtained regarding highly radiative shocks (RSs) generated in a low-density gas filled cell on the GEKKO XII laser facility. The RS was generated by using an ablator-pusher two-layer target (CH/Sn) and a propagation medium (Xe). High velocity RSs have been generated (100–140 km/s), while limiting as much as possible the preheating produced by the corona emission. Both self-emission and visible probe diagnostics highlighted a strong emission in the shock and an electron density in the downstream gas. The RS characteristics that depend on the initial conditions are described here as well as its precursor interaction with an aluminium foil used as an obstacle. The obtained results are discussed which show a strong extension of the radiative precursor (1 mm) leading to an expansion velocity of the obstacle up to ≈30 km/s compatible to a 20 eV temperature.
Journal of Synchrotron Radiation | 2017
M. Ruiz-Lopez; Anatoly Ya. Faenov; T. A. Pikuz; Norio Ozaki; A. Mitrofanov; B. Albertazzi; N. J. Hartley; Toshimasa Matsuoka; R. Ochante; Yoshinori Tange; T. Yabuuchi; T. Habara; K. A. Tanaka; Yuichi Inubushi; Makina Yabashi; Masaharu Nishikino; Tetsuya Kawachi; Sergey A. Pikuz; Tetsuya Ishikawa; R. Kodama; D. Bleiner
Direct metrology of coherent short-wavelength beamlines is important for obtaining operational beam characteristics at the experimental site. However, since beam-time limitation imposes fast metrology procedures, a multi-parametric metrology from as low as a single shot is desirable. Here a two-dimensional (2D) procedure based on high-resolution Fresnel diffraction analysis is discussed and applied, which allowed an efficient and detailed beamline characterization at the SACLA XFEL. So far, the potential of Fresnel diffraction for beamline metrology has not been fully exploited because its high-frequency fringes could be only partly resolved with ordinary pixel-limited detectors. Using the high-spatial-frequency imaging capability of an irradiated LiF crystal, 2D information of the coherence degree, beam divergence and beam quality factor M2 were retrieved from simple diffraction patterns. The developed beam metrology was validated with a laboratory reference laser, and then successfully applied at a beamline facility, in agreement with the source specifications.
Journal of Applied Physics | 2016
Tatiana A. Pikuz; A. Ya. Faenov; Norimasa Ozaki; N. J. Hartley; B. Albertazzi; Toshimasa Matsuoka; Kouhei Takahashi; H. Habara; Yoshinori Tange; Satoshi Matsuyama; Kazuto Yamauchi; R. Ochante; Keiichi Sueda; Osami Sakata; Toshimori Sekine; Tomoko Sato; Yuhei Umeda; Yuichi Inubushi; T. Yabuuchi; Tadashi Togashi; Tetsuo Katayama; Makina Yabashi; M. Harmand; G. Morard; M. Koenig; V. V. Zhakhovsky; N. A. Inogamov; A.S. Safronova; A. Stafford; I. Yu. Skobelev
We present an indirect method of estimating the strength of a shock wave, allowing on line monitoring of its reproducibility in each laser shot. This method is based on a shot-to-shot measurement of the X-ray emission from the ablated plasma by a high resolution, spatially resolved focusing spectrometer. An optical pump laser with energy of 1.0 J and pulse duration of similar to 660 ps was used to irradiate solid targets or foils with various thicknesses containing Oxygen, Aluminum, Iron, and Tantalum. The high sensitivity and resolving power of the X-ray spectrometer allowed spectra to be obtained on each laser shot and to control fluctuations of the spectral intensity emitted by different plasmas with an accuracy of similar to 2%, implying an accuracy in the derived electron plasma temperature of 5%-10% in pump-probe high energy density science experiments. At nano-and sub-nanosecond duration of laser pulse with relatively low laser intensities and ratio Z/A similar to 0.5, the electron temperature follows T-e similar to I-las(2/3). Thus, measurements of the electron plasma temperature allow indirect estimation of the laser flux on the target and control its shot-to-shot fluctuation. Knowing the laser flux intensity and its fluctuation gives us the possibility of monitoring shot-to-shot reproducibility of shock wave strength generation with high accuracy. Published by AIP Publishing.
Physics of Plasmas | 2015
B. Albertazzi; Shihua Chen; P. Antici; J. Böker; M. Borghesi; J. Breil; V. Dervieux; J. L. Feugeas; L. Lancia; M. Nakatsutsumi; Ph. Nicolaï; L. Romagnagni; R. Shepherd; Y. Sentoku; Mikhail V. Starodubtsev; Marco Swantusch; V. T. Tikhonchuk; O. Willi; Emmanuel D'Humieres; H. Pépin; J. Fuchs
The dynamics of self-generated magnetic B-fields produced following the interaction of a high contrast, high intensity (I > 1019 W cm−2) laser beam with thin (3 μm thick) solid (Al or Au) targets is investigated experimentally and numerically. Two main sources drive the growth of B-fields on the target surfaces. B-fields are first driven by laser-generated hot electron currents that relax over ∼10–20 ps. Over longer timescales, the hydrodynamic expansion of the bulk of the target into vacuum also generates B-field induced by non-collinear gradients of density and temperature. The laser irradiation of the target front side strongly localizes the energy deposition at the target front, in contrast to the target rear side, which is heated by fast electrons over a much larger area. This induces an asymmetry in the hydrodynamic expansion between the front and rear target surfaces, and consequently the associated B-fields are found strongly asymmetric. The sole long-lasting (>30 ps) B-fields are the ones growing...
International Conference on X-ray Lasers | 2016
Tatiana A. Pikuz; A. Ya. Faenov; Toshimasa Matsuoka; B. Albertazzi; Norio Ozaki; N. Hartely; O. Muray Ricardo Arturo; T. Yabuuchi; H. Habara; Satoshi Matsuyama; Kazuto Yamauchi; Yuichi Inubushi; Tadashi Togashi; Hirokatsu Yumoto; Yoshinori Tange; Kensuke Tono; Yuya Sato; Makina Yabashi; Masaharu Nishikino; Tetsuya Kawachi; Alexander Mitrofanov; S. A. Pikuz; D. Bleiner; A N Grum-Grzhimailo; N. N. Rosanov; N. V. Vysotina; M. Harmand; M. Koenig; K. A. Tanaka; Tetsuya Ishikawa
We present here a new diagnostics based on using LiF crystal detectors that are able to perform measurements an intensity distribution of X-rays beams with diameters ranging from some microns up to some centimetres with high spatial resolution (~1 µm). In situ, 3D visualization of SACLA XFEL focused beam profile along propagation, including propagation inside photoluminescence solid materials, is demonstrated. Also, a high spatial resolution control a quality of targets used in optical laser pump—XFEL probe HEDS experiments is proposed.