21 results on '"Ichinohe, Yuto"'
Search Results
2. Reconstruction of multiple Compton scattering events in MeV gamma-ray Compton telescopes towards GRAMS: The physics-based probabilistic model
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Yoneda, Hiroki, Odaka, Hirokazu, Ichinohe, Yuto, Takashima, Satoshi, Aramaki, Tsuguo, Aoyama, Kazutaka, Asaadi, Jonathan, Fabris, Lorenzo, Inoue, Yoshiyuki, Karagiorgi, Georgia, Khangulyan, Dmitry, Kimura, Masato, Leyva, Jonathan, Mukherjee, Reshmi, Nakasone, Taichi, Perez, Kerstin, Sakurai, Mayu, Seligman, William, Tanaka, Masashi, Tsuji, Naomi, Yorita, Kohei, and Zeng, Jiancheng
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- 2023
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3. Event reconstruction of Compton telescopes using a multi-task neural network
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Takashima, Satoshi, Odaka, Hirokazu, Yoneda, Hiroki, Ichinohe, Yuto, Bamba, Aya, Aramaki, Tsuguo, and Inoue, Yoshiyuki
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- 2022
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4. Performance study of a large CsI(Tl) scintillator with an MPPC readout for nanosatellites used to localize gamma-ray bursts
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Torigoe, Kento, Fukazawa, Yasushi, Galgóczi, Gabór, Mizuno, Tsunefumi, Nakazawa, Kazuhiro, Ohno, Masanori, Pál, András, Takahashi, Hiromitsu, Tanaka, Koji, Tarcai, Norbert, Uchida, Nagomi, Werner, Norbert, Enoto, Teruaki, Frei, Zsolt, Ichinohe, Yuto, Kiss, László, Odaka, Hirokazu, Řípa, Jakub, and Várhegyi, Zsolt
- Published
- 2019
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5. Application of transition-edge sensors for micro-X-ray fluorescence measurements and micro-X-ray absorption near edge structure spectroscopy: a case study of uranium speciation in biotite obtained from a uranium mine.
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Yomogida, Takumi, Hashimoto, Tadashi, Okumura, Takuma, Yamada, Shinya, Tatsuno, Hideyuki, Noda, Hirofumi, Hayakawa, Ryota, Okada, Shinji, Takatori, Sayuri, Isobe, Tadaaki, Hiraki, Takahiro, Sato, Toshiki, Toyama, Yuichi, Ichinohe, Yuto, Sekizawa, Oki, Nitta, Kiyofumi, Kurihara, Yuichi, Fukushima, Shigeru, Uruga, Tomoya, and Kitatsuji, Yoshihiro
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X-ray absorption near edge structure ,URANIUM mining ,CHEMICAL speciation ,BIOTITE ,X-ray spectra ,URANIUM - Abstract
In this study, we successfully applied a transition-edge sensor (TES) spectrometer as a detector for microbeam X-ray measurements from a synchrotron X-ray light source in the hard X-ray region to determine uranium (U) distribution at the micro-scale and its chemical species in biotite obtained from a U mine. It is difficult to separate the fluorescent X-ray of the U Lα
1 line at 13.615 keV from that of the Rb Kα line at 13.395 keV in the X-ray fluorescence spectrum with an energy resolution of approximately 220 eV using a conventional silicon drift detector (SDD). Meanwhile, the fluorescent X-rays of U Lα1 and Rb Kα were fully separated by a TES with 50 eV energy resolution at an energy of around 13 keV. The successful peak separation by the TES led to an accurate mapping analysis of trace U in micro-X-ray fluorescence measurements and a decrease in the signal-to-background ratio in micro-X-ray absorption near edge structure spectroscopy. Thus, it could be a powerful tool for studying the U distribution and speciation in various environmental samples. [ABSTRACT FROM AUTHOR]- Published
- 2024
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6. Study of the polarimetric performance of a Si/CdTe semiconductor Compton camera for the Hitomi satellite
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Katsuta, Junichiro, Edahiro, Ikumi, Watanabe, Shin, Odaka, Hirokazu, Uchida, Yusuke, Uchida, Nagomi, Mizuno, Tsunefumi, Fukazawa, Yasushi, Hayashi, Katsuhiro, Habata, Sho, Ichinohe, Yuto, Kitaguchi, Takao, Ohno, Masanori, Ohta, Masayuki, Takahashi, Hiromitsu, Takahashi, Tadayuki, Takeda, Shin'ichiro, Tajima, Hiroyasu, Yuasa, Takayuki, and Itou, Masayoshi
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- 2016
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7. The first demonstration of the concept of “narrow-FOV Si/CdTe semiconductor Compton camera”
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Ichinohe, Yuto, Uchida, Yuusuke, Watanabe, Shin, Edahiro, Ikumi, Hayashi, Katsuhiro, Kawano, Takafumi, Ohno, Masanori, Ohta, Masayuki, Takeda, Shin׳ichiro, Fukazawa, Yasushi, Katsuragawa, Miho, Nakazawa, Kazuhiro, Odaka, Hirokazu, Tajima, Hiroyasu, Takahashi, Hiromitsu, Takahashi, Tadayuki, and Yuasa, Takayuki
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- 2016
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8. A portable Si/CdTe Compton camera and its applications to the visualization of radioactive substances
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Takeda, Shin׳ichiro, Harayama, Atsushi, Ichinohe, Yuto, Odaka, Hirokazu, Watanabe, Shin, Takahashi, Tadayuki, Tajima, Hiroyasu, Genba, Kei, Matsuura, Daisuke, Ikebuchi, Hiroshi, Kuroda, Yoshikatsu, and Tomonaka, Tetsuya
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- 2015
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9. The Si/CdTe semiconductor Compton camera of the ASTRO-H Soft Gamma-ray Detector (SGD)
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Watanabe, Shin, Tajima, Hiroyasu, Fukazawa, Yasushi, Ichinohe, Yuto, Takeda, Shin׳ichiro, Enoto, Teruaki, Fukuyama, Taro, Furui, Shunya, Genba, Kei, Hagino, Kouichi, Harayama, Atsushi, Kuroda, Yoshikatsu, Matsuura, Daisuke, Nakamura, Ryo, Nakazawa, Kazuhiro, Noda, Hirofumi, Odaka, Hirokazu, Ohta, Masayuki, Onishi, Mitsunobu, Saito, Shinya, Sato, Goro, Sato, Tamotsu, Takahashi, Tadayuki, Tanaka, Takaaki, Togo, Atsushi, and Tomizuka, Shinji
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- 2014
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10. Solar abundance ratios of the iron-peak elements in the Perseus cluster
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Aharonian, Felix, Akamatsu, Hiroki, Akimoto, Fumie, Allen, Steven W., Angelini, Lorella, Audard, Marc, Awaki, Hisamitsu, Axelsson, Magnus, Bamba, Aya, Bautz, Marshall W., Blandford, Roger, Brenneman, Laura W., Brown, Gregory V., Bulbul, Esra, Cackett, Edward M., Chernyakova, Maria, Chiao, Meng P., Coppi, Paolo S., Costantini, Elisa, de Plaa, Jelle, den Herder, Jan-Willem, Done, Chris, Dotani, Tadayasu, Ebisawa, Ken, Eckart, Megan E., Enoto, Teruaki, Ezoe, Yuichiro, Fabian, Andrew C., Ferrigno, Carlo, Foster, Adam R., Fujimoto, Ryuichi, Fukazawa, Yasushi, Furuzawa, Akihiro, Galeazzi, Massimiliano, Gallo, Luigi C., Gandhi, Poshak, Giustini, Margherita, Goldwurm, Andrea, Gu, Liyi, Guainazzi, Matteo, Haba, Yoshito, Hagino, Kouichi, Hamaguchi, Kenji, Harrus, Ilana M., Hatsukade, Isamu, Hayashi, Katsuhiro, Hayashi, Takayuki, Hayashida, Kiyoshi, Hiraga, Junko S., Hornschemeier, Ann, Hoshino, Akio, Hughes, John P., Ichinohe, Yuto, Iizuka, Ryo, Inoue, Hajime, Inoue, Yoshiyuki, Ishida, Manabu, Ishikawa, Kumi, Ishisaki, Yoshitaka, Iwai, Masachika, Kaastra, Jelle, Kallman, Tim, Kamae, Tsuneyoshi, Kataoka, Jun, Katsuda, Satoru, Kawai, Nobuyuki, Kelley, Richard L., Kilbourne, Caroline A., Kitaguchi, Takao, Kitamoto, Shunji, Kitayama, Tetsu, Kohmura, Takayoshi, Kokubun, Motohide, Koyama, Katsuji, Koyama, Shu, Kretschmar, Peter, Krimm, Hans A., Kubota, Aya, Kunieda, Hideyo, Laurent, Philippe, Lee, Shiu-Hang, Leutenegger, Maurice A., Limousine, Olivier, Loewenstein, Michael, Long, Knox S., Lumb, David, Madejski, Greg, Maeda, Yoshitomo, Maier, Daniel, Makishima, Kazuo, Markevitch, Maxim, Matsumoto, Hironori, Matsushita, Kyoko, McCammon, Dan, McNamara, Brian R., Mehdipour, Missagh, Miller, Eric D., Miller, Jon M., Mineshige, Shin, Mitsuda, Kazuhisa, Mitsuishi, Ikuyuki, Miyazawa, Takuya, Mizuno, Tsunefumi, Mori, Hideyuki, Mori, Koji, Mukai, Koji, Murakami, Hiroshi, Mushotzky, Richard F., Nakagawa, Takao, Nakajima, Hiroshi, Nakamori, Takeshi, Nakashima, Shinya, Nakazawa, Kazuhiro, Nobukawa, Kumiko K., Nobukawa, Masayoshi, Noda, Hirofumi, Odaka, Hirokazu, Ohashi, Takaya, Ohno, Masanori, Okajima, Takashi, Ota, Naomi, Ozaki, Masanobu, Paerels, Frits, Paltani, Stéphane, Petre, Robert, Pinto, Ciro, Porter, Frederick S., Pottschmidt, Katja, Reynolds, Christopher S., Safi-Harb, Samar, Saito, Shinya, Sakai, Kazuhiro, Sasaki, Toru, Sato, Goro, Sato, Kosuke, Sato, Rie, Sawada, Makoto, Schartel, Norbert, Serlemitsos, Peter J., Seta, Hiromi, Shidatsu, Megumi, Simionescu, Aurora, Smith, Randall K., Soong, Yang, Stawarz, Lukasz, Sugawara, Yasuharu, Sugita, Satoshi, Szymkowiak, Andrew, Tajima, Hiroyasu, Takahashi, Hiromitsu, Takahashi, Tadayuki, Takeda, Shinʼichiro, Takei, Yoh, Tamagawa, Toru, Tamura, Takayuki, Tanaka, Takaaki, Tanaka, Yasuo, Tanaka, Yasuyuki T., Tashiro, Makoto S., Tawara, Yuzuru, Terada, Yukikatsu, Terashima, Yuichi, Tombesi, Francesco, Tomida, Hiroshi, Tsuboi, Yohko, Tsujimoto, Masahiro, Tsunemi, Hiroshi, Go Tsuru, Takeshi, Uchida, Hiroyuki, Uchiyama, Hideki, Uchiyama, Yasunobu, Ueda, Shutaro, Ueda, Yoshihiro, Uno, Shinʼichiro, Urry, Megan C., Ursino, Eugenio, de Vries, Cor P., Watanabe, Shin, Werner, Norbert, Wik, Daniel R., Wilkins, Dan R., Williams, Brian J., Yamada, Shinya, Yamaguchi, Hiroya, Yamaoka, Kazutaka, Yamasaki, Noriko Y., Yamauchi, Makoto, Yamauchi, Shigeo, Yaqoob, Tahir, Yatsu, Yoichi, Yonetoku, Daisuke, Zhuravleva, Irina, and Zoghbi, Abderahmen
- Published
- 2017
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11. High-resolution Compton cameras based on Si/CdTe double-sided strip detectors
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Odaka, Hirokazu, Ichinohe, Yuto, Takeda, Shin'ichiro, Fukuyama, Taro, Hagino, Koichi, Saito, Shinya, Sato, Tamotsu, Sato, Goro, Watanabe, Shin, Kokubun, Motohide, Takahashi, Tadayuki, Yamaguchi, Mitsutaka, Tanaka, Takaaki, Tajima, Hiroyasu, Nakazawa, Kazuhiro, and Fukazawa, Yasushi
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- 2012
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12. Applications and Imaging Techniques of a Si/CdTe Compton Gamma-Ray Camera
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Takeda, Shin’ichiro, Ichinohe, Yuto, Hagino, Kouichi, Odaka, Hirokazu, Yuasa, Takayuki, Ishikawa, Shin-nosuke, Fukuyama, Taro, Saito, Shinya, Sato, Tamotsu, Sato, Goro, Watanabe, Shin, Kokubun, Motohide, Takahashi, Tadayuki, Yamaguchi, Mitsutaka, Tajima, Hiroyasu, Tanaka, Takaaki, Nakazawa, Kazuhiro, Fukazawa, Yasushi, and Nakano, Takashi
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- 2012
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13. Galaxy clusters at z ∼ 1 imaged by ALMA with the Sunyaev–Zel'dovich effect.
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Kitayama, Tetsu, Ueda, Shutaro, Okabe, Nobuhiro, Akahori, Takuya, Hilton, Matt, Hughes, John P, Ichinohe, Yuto, Kohno, Kotaro, Komatsu, Eiichiro, Lin, Yen-Ting, Miyatake, Hironao, Oguri, Masamune, Sifón, Cristóbal, Takakuwa, Shigehisa, Takizawa, Motokazu, Tsutsumi, Takahiro, Marrewijk, Joshiwa van, and Wollack, Edward J
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SUNYAEV-Zel'dovich effect ,GALAXY clusters ,ELECTRON distribution ,ANGULAR measurements ,PHYSICAL cosmology - Abstract
We present high angular resolution measurements of the thermal Sunyaev–Zel'dovich effect (SZE) toward two galaxy clusters, RCS J2319+0038 at |$z$| = 0.9 and HSC J0947−0119 at |$z$| = 1.1, by the Atacama Large Millimeter/submillimeter Array (ALMA) in Band 3. They are supplemented with available Chandra X-ray data, optical data taken by Hyper Suprime-Cam on Subaru, and millimeter-wave SZE data from the Atacama Cosmology Telescope. Taking into account departures from spherical symmetry, we have reconstructed non-parametrically the inner pressure profile of two clusters as well as electron temperature and density profiles for RCS J2319+0038. This is one of the first such measurements for an individual cluster at |$z \gtrsim 0.9$|. We find that the inner pressure profile of both clusters is much shallower than that of local cool-core clusters. Our results consistently suggest that RCS J2319+0038 hosts a weak cool core, where radiative cooling is less significant than in local cool cores. On the other hand, HSC J0947−0119 exhibits an even shallower pressure profile than RCS J2319+0038 and is more likely to be a non-cool-core cluster. The SZE centroid position is offset by more than 140 |$h_{70}^{-1}$| kpc from the peaks of galaxy distribution in HSC J0947−0119, suggesting a stronger influence of mergers in this cluster. We conclude that these distant clusters are at a very early stage of developing the cool cores typically found in clusters at lower redshifts. [ABSTRACT FROM AUTHOR]
- Published
- 2023
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14. X-ray hot spots in the eastern ear of the supernova remnant W 50 and the microquasar SS 433 system.
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Hayakawa, Ryota, Yamada, Shinya, Suda, Hirotaka, Ichinohe, Yuto, Higurashi, Ryota, Sakemi, Haruka, Machida, Mami, Ohmura, Takumi, Katsuda, Satoru, Uchiyama, Hideki, Sato, Toshiki, Akamatsu, Hiroki, and Axelsson, Magnus
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INVERSE Compton scattering ,SUPERNOVA remnants ,SPECTRAL energy distribution ,MAGNETIC flux density ,X-rays ,GAMMA rays - Abstract
We examined the X-ray and radio spatial structure at the eastern ear of the W 50/SS 433 system to clarify a characteristic feature of the termination region of the SS 433 jet, and found that a hot spot ahead of the filament structure, which is considered to be a terminal shock of the SS 433 eastern jet, is clearly different from a single point source. The detailed spatial structure of the X-ray emission is finely resolved by Chandra observations, showing that there are two sources. By comparing the point-spread function of Chandra with the radial profiles of the two sources, the northern one is clearly more extended than a point source while the other seems marginally extended. Since there are no point sources nearby, the northern hot spot is likely a localized diffuse source. The northern hot spot spatially corresponds to the peak of the radio emission. Its spatial correlation is confirmed by an X-ray image using XMM-Newton. The X-ray spectra of the two sources are reproduced by a single absorbed power-law but the column density of the northern part is larger by a factor of ∼3. When a radiation model comprising synchrotron emission and inverse Compton emission is applied to the spectral energy distribution of the northern hot spot, the emission from this spot can be explained by the radiation from an electron population accelerated up to 30 TeV in a magnetic field strength of B ≲ 50 μG. This model also agrees with the radio and X-ray data, as well as the upper limit of gamma-ray emission obtained by the Fermi satellite. [ABSTRACT FROM AUTHOR]
- Published
- 2022
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15. Broadband high-energy resolution hard x-ray spectroscopy using transition edge sensors at SPring-8.
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Yamada, Shinya, Ichinohe, Yuto, Tatsuno, Hideyuki, Hayakawa, Ryota, Suda, Hirotaka, Ohashi, Takaya, Ishisaki, Yoshitaka, Uruga, Tomoya, Sekizawa, Oki, Nitta, Kiyofumi, Takahashi, Yoshio, Itai, Takaaki, Suga, Hiroki, Nagasawa, Makoto, Tanaka, Masato, Kurisu, Minako, Hashimoto, Tadashi, Bennett, Douglas, Denison, Ed, and Doriese, William Bertrand
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HARD X-rays , *X-ray spectroscopy , *HIGH resolution spectroscopy , *FLUORIMETRY , *X-ray spectra , *MICROBIOLOGICAL aerosols , *X-ray absorption near edge structure - Abstract
We have succeeded in operating a transition-edge sensor (TES) spectrometer and evaluating its performance at the SPring-8 synchrotron x-ray light source. The TES spectrometer consists of a 240 pixel National Institute of Standards and Technology (NIST) TES system, and 220 pixels are operated simultaneously with an energy resolution of 4 eV at 6 keV at a rate of ∼1 c/s pixel−1. The tolerance for high count rates is evaluated in terms of energy resolution and live time fraction, leading to an empirical compromise of ∼2 × 103 c/s (all pixels) with an energy resolution of 5 eV at 6 keV. By utilizing the TES's wideband spectroscopic capability, simultaneous multi-element analysis is demonstrated for a standard sample. We conducted x-ray absorption near-edge structure (XANES) analysis in fluorescence mode using the TES spectrometer. The excellent energy resolution of the TES enabled us to detect weak fluorescence lines from dilute samples and trace elements that have previously been difficult to resolve due to the nearly overlapping emission lines of other dominant elements. The neighboring lines of As Kα and Pb Lα2 of the standard sample were clearly resolved, and the XANES of Pb Lα2 was obtained. Moreover, the x-ray spectrum from the small amount of Fe in aerosols was distinguished from the spectrum of a blank target, which helps us to understand the targets and the environment. These results are the first important step for the application of high resolution TES-based spectroscopy at hard x-ray synchrotron facilities. [ABSTRACT FROM AUTHOR]
- Published
- 2021
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16. X-ray study of the double source plane gravitational lens system Eye of Horus observed with XMM–Newton.
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Tanaka, Keigo, Tsuji, Ayumi, Akamatsu, Hiroki, Chan, J H H, Coupon, Jean, Egami, Eiichi, Finet, Francois, Fujimoto, Ryuichi, Ichinohe, Yuto, Jaelani, Anton T, Lee, Chien-Hsiu, Mitsuishi, Ikuyuki, More, Anupreeta, More, Surhud, Oguri, Masamune, Okabe, Nobuhiro, Ota, Naomi, Rusu, Cristian E, Sonnenfeld, Alessandro, and Tanaka, Masayuki
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GRAVITATIONAL lenses ,HYDROSTATIC equilibrium ,EYE ,X-rays ,GALAXY clusters - Abstract
A double source plane (DSP) system is a precious probe for the density profile of distant galaxies and cosmological parameters. However, these measurements could be affected by the surrounding environment of the lens galaxy. Thus, it is important to evaluate the cluster-scale mass for detailed mass modelling. We observed the Eye of Horus , a DSP system discovered by the Hyper Suprime-Cam Subaru Strategic Survey (HSC–SSP), with XMM–Newton. We detected two X-ray extended emissions, originating from two clusters, one centred at the Eye of Horus , and the other located ∼100 arcsec north-east to the Eye of Horus. We determined the dynamical mass assuming hydrostatic equilibrium, and evaluated their contributions to the lens mass interior of the Einstein radius. The contribution of the former cluster is |$1.1^{+1.2}_{-0.5}\times 10^{12}\, \mathrm{M}_{\odot }$| , which is |$21\!-\!76{{\ \rm per\ cent}}$| of the total mass within the Einstein radius. The discrepancy is likely due to the complex gravitational structure along the line of sight. On the other hand, the contribution of the latter cluster is only |$\sim 2{{\ \rm per\ cent}}$| on the Eye of Horus. Therefore, the influence associated with this cluster can be ignored. [ABSTRACT FROM AUTHOR]
- Published
- 2020
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17. X-ray study of spatial structures in Tycho's supernova remnant using unsupervised deep learning.
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Iwasaki, Hiroyoshi, Ichinohe, Yuto, and Uchiyama, Yasunobu
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SUPERNOVA remnants , *GAUSSIAN mixture models , *X-rays , *IRON powder , *MACHINE learning , *GALAXY clusters , *DEEP learning - Abstract
Recent rapid development of deep learning algorithms, which can implicitly capture structures in high-dimensional data, opens a new chapter in astronomical data analysis. We report here a new implementation of deep learning techniques for X-ray analysis. We apply a variational autoencoder (VAE) using a deep neural network for spatio-spectral analysis of data obtained by Chandra X-ray Observatory from Tycho 's supernova remnant (SNR). We established an unsupervised learning method combining the VAE and a Gaussian mixture model (GMM), where the dimensions of the observed spectral data are reduced by the VAE, and clustering in feature space is performed by the GMM. We found that some characteristic spatial structures, such as the iron knot on the eastern rim, can be automatically recognized by this method, which uses only spectral properties. This result shows that unsupervised machine learning can be useful for extracting characteristic spatial structures from spectral information in observational data (without detailed spectral analysis), which would reduce human-intensive preprocessing costs for understanding fine structures in diffuse astronomical objects, e.g. SNRs or galaxy clusters. Such data-driven analysis can be used to select regions from which to extract spectra for detailed analysis and help us make the best use of the large amount of spectral data available currently and arriving in the coming decades. [ABSTRACT FROM AUTHOR]
- Published
- 2019
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18. Estimation of the detected background by the future gamma ray transient mission CAMELOT.
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Řípa, Jakub, Galgóczi, Gábor, Werner, Norbert, Pál, András, Ohno, Masanori, Mészáros, László, Mizuno, Tsunefumi, Tarcai, Norbert, Torigoe, Kento, Uchida, Nagomi, Fukazawa, Yasushi, Takahashi, Hiromitsu, Nakazawa, Kazuhiro, Hirade, Naoyoshi, Hirose, Kengo, Hisadomi, Syohei, Enoto, Teruaki, Odaka, Hirokazu, Ichinohe, Yuto, and Frei, Zsolt
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GAMMA rays ,GRAVITATIONAL waves ,GAMMA ray bursts ,ASTROPHYSICAL radiation ,SPACE environment ,MAGNETARS ,COSMIC rays ,GAMMA ray spectrometry - Abstract
This study presents a background estimation for the CubeSats Applied for MEasuring and LOcalising Transients (CAMELOT), which is a proposed fleet of nanosatellites for the all‐sky monitoring and timing‐based localization of gamma ray transients with precise localization capability at low Earth orbits. CAMELOT will allow us to observe and precisely localize short gamma ray bursts (GRBs) associated with kilonovae, long GRBs associated with core‐collapse massive stars, magnetar outbursts, terrestrial gamma ray flashes, and gamma ray counterparts to gravitational wave sources. A fleet of at least nine 3U CubeSats is proposed to be equipped with large and thin CsI(Tl) scintillators read out by multipixel photon counters (MPPC). A careful study of the radiation environment in space is necessary to optimize the detector casing, estimate the duty cycle due to the crossing of the South Atlantic Anomaly and polar regions, and minimize the effect of the radiation damage of MPPCs. [ABSTRACT FROM AUTHOR]
- Published
- 2019
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19. Simulations of expected signal and background of gamma-ray sources by large field-of-view detectors aboard CubeSats.
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Galgóczi, Gábor, Řípa, Jakub, Campana, Riccardo, Werner, Norbert, Pál, András, Ohno, Masanori, Mészáros, László, Mizuno, Tsunefumi, Tarcai, Norbert, Torigoe, Kento, Uchida, Nagomi, Fukazawa, Yasushi, Takahashi, Hiromitsu, Nakazawa, Kazuhiro, Hirade, Naoyoshi, Hirose, Kengo, Hisadomi, Syohei, Enoto, Teruaki, Odaka, Hirokazu, and Ichinohe, Yuto
- Published
- 2021
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20. X-ray properties of high-richness CAMIRA clusters in the Hyper Suprime-Cam Subaru Strategic Program field.
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Ota, Naomi, Mitsuishi, Ikuyuki, Babazaki, Yasunori, Akamatsu, Hiroki, Ichinohe, Yuto, Ueda, Shutaro, Okabe, Nobuhiro, Oguri, Masamune, Fujimoto, Ryuichi, Hamana, Takashi, Miyaoka, Keita, Miyazaki, Satoshi, Otani, Hanae, Tanaka, Keigo, Tsuji, Ayumi, and Yoshida, Atsushi
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X-rays ,GALAXY clusters ,DISTRIBUTION (Probability theory) ,CLUSTER sampling ,X-ray imaging - Abstract
We present the first results of a pilot X-ray study of 37 rich galaxy clusters at 0.1 < z < 1.1 in the Hyper Suprime-Cam Subaru Strategic Program field. Diffuse X-ray emissions from these clusters were serendipitously detected in the XMM-Newton fields of view. We systematically analyze X-ray images of 37 clusters and emission spectra of a subsample of 17 clusters with high photon statistics by using the XMM-Newton archive data. The frequency distribution of the offset between the X-ray centroid or peak and the position of the brightest cluster galaxy was derived for the optical cluster sample. The fraction of relaxed clusters estimated from the X-ray peak offsets in 17 clusters is 29 ± 11(±13)%, which is smaller than that of the X-ray cluster samples such as HIFLUGCS. Since the optical cluster search is immune to the physical state of X-ray-emitting gas, it is likely to cover a larger range of the cluster morphology. We also derive the luminosity–temperature relation and found that the slope is marginally shallower than those of X-ray-selected samples and consistent with the self-similar model prediction of 2. Accordingly, our results show that the X-ray properties of the optical clusters are marginally different from those observed in the X-ray samples. The implication of the results and future prospects are briefly discussed. [ABSTRACT FROM AUTHOR]
- Published
- 2020
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21. Hitomi X-ray studies of Giant Radio Pulses from the Crab pulsar.
- Author
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Aharonian F, Akamatsu H, Akimoto F, Allen SW, Angelini L, Audard M, Awaki H, Axelsson M, Bamba A, Bautz MW, Blandford R, Brenneman LW, Brown GV, Bulbul E, Cackett EM, Chernyakova M, Chiao MP, Coppi PS, Costantini E, De Plaa J, De Vries CP, Den Herder JW, Done C, Dotani T, Ebisawa K, Eckart ME, Enoto T, Ezoe Y, Fabian AC, Ferrigno C, Foster AR, Fujimoto R, Fukazawa Y, Furuzawa A, Galeazzi M, Gallo LC, Gandhi P, Giustini M, Goldwurm A, Gu L, Guainazzi M, Haba Y, Hagino K, Hamaguchi K, Harrus IM, Hatsukade I, Hayashi K, Hayashi T, Hayashida K, Hiraga JS, Hornschemeier A, Hoshino A, Hughes JP, Ichinohe Y, Iizuka R, Inoue H, Inoue Y, Ishida M, Ishikawa K, Ishisaki Y, Iwai M, Kaastra J, Kallman T, Kamae T, Kataoka J, Katsuda S, Kawai N, Kelley RL, Kilbourne CA, Kitaguchi T, Kitamoto S, Kitayama T, Kohmura T, Kokubun M, Koyama K, Koyama S, Kretschmar P, Krimm HA, Kubota A, Kunieda H, Laurent P, Lee SH, Leutenegger MA, Limousin OO, Loewenstein M, Long KS, Lumb D, Madejski G, Maeda Y, Maier D, Makishima K, Markevitch M, Matsumoto H, Matsushita K, Mccammon D, Mcnamara BR, Mehdipour M, Miller ED, Miller JM, Mineshige S, Mitsuda K, Mitsuishi I, Miyazawa T, Mizuno T, Mori H, Mori K, Mukai K, Murakami H, Mushotzky RF, Nakagawa T, Nakajima H, Nakamori T, Nakashima S, Nakazawa K, Nobukawa KK, Nobukawa M, Noda H, Odaka H, Ohashi T, Ohno M, Okajima T, Oshimizu K, Ota N, Ozaki M, Paerels F, Paltani S, Petre R, Pinto C, Porter FS, Pottschmidt K, Reynolds CS, Safi-Harb S, Saito S, Sakai K, Sasaki T, Sato G, Sato K, Sato R, Sawada M, Schartel N, Serlemtsos PJ, Seta H, Shidatsu M, Simionescu A, Smith RK, Soong Y, Stawarz Ł, Sugawara Y, Sugita S, Szymkowiak A, Tajima H, Takahashi H, Takahashi T, Takeda S, Takei Y, Tamagawa T, Tamura T, Tanaka T, Tanaka Y, Tanaka YT, Tashiro MS, Tawara Y, Terada Y, Terashima Y, Tombesi F, Tomida H, Tsuboi Y, Tsujimoto M, Tsunemi H, Tsuru TG, Uchida H, Uchiyama H, Uchiyama Y, Ueda S, Ueda Y, Uno S, Urry CM, Ursino E, Watanabe S, Werner N, Wilkins DR, Williams BJ, Yamada S, Yamaguchi H, Yamaoka K, Yamasaki NY, Yamauchi M, Yamauchi S, Yaqoob T, Yatsu Y, Yonetoku D, Zhuravleva I, Zoghbi A, Terasawa T, Sekido M, Takefuji K, Kawai E, Misawa H, Tsuchiya F, Yamazaki R, Kobayashi E, Kisaka S, and Aoki T
- Abstract
To search for giant X-ray pulses correlated with the giant radio pulses (GRPs) from the Crab pulsar, we performed a simultaneous observation of the Crab pulsar with the X-ray satellite Hitomi in the 2 - 300 keV band and the Kashima NICT radio observatory in the 1.4 - 1.7 GHz band with a net exposure of about 2 ks on 25 March 2016, just before the loss of the Hitomi mission. The timing performance of the Hitomi instruments was confirmed to meet the timing requirement and about 1,000 and 100 GRPs were simultaneously observed at the main and inter-pulse phases, respectively, and we found no apparent correlation between the giant radio pulses and the X-ray emission in either the main or inter-pulse phases. All variations are within the 2 sigma fluctuations of the X-ray fluxes at the pulse peaks, and the 3 sigma upper limits of variations of main- or inter-pulse GRPs are 22% or 80% of the peak flux in a 0.20 phase width, respectively, in the 2 - 300 keV band. The values become 25% or 110% for main or inter-pulse GRPs, respectively, when the phase width is restricted into the 0.03 phase. Among the upper limits from the Hitomi satellite, those in the 4.5-10 keV and the 70-300 keV are obtained for the first time, and those in other bands are consistent with previous reports. Numerically, the upper limits of main- and inter-pulse GRPs in the 0.20 phase width are about (2.4 and 9.3) ×10
-11 erg cm-2 , respectively. No significant variability in pulse profiles implies that the GRPs originated from a local place within the magnetosphere and the number of photon-emitting particles temporally increases. However, the results do not statistically rule out variations correlated with the GRPs, because the possible X-ray enhancement may appear due to a > 0.02% brightening of the pulse-peak flux under such conditions.- Published
- 2018
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