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Your search keyword '"Fujita, Ryuichi"' showing total 7 results
Start Over Author "Fujita, Ryuichi" Publisher american physical society
7 results on '"Fujita, Ryuichi"'

1. Observation results by the TAMA300 detector on gravitational wave bursts from stellar-core collapses

Author

Ando, Masaki, Kojima, Yasufumi, Arai, Koji, Aso, Youichi, Beyersdorf, Peter, Hayama, Kazuhiro, Iida, Yukiyoshi, Kanda, Nobuyuki, Kawamura, Seiji, Kondo, Kazuhiro, Mio, Norikatsu, Miyoki, Shinji, Moriwaki, Shigenori, Nagano, Shigeo, Numata, Kenji, Sato, Shuichi, Somiya, Kentaro, Tagoshi, Hideyuki, Takahashi, Hirotaka, Takahashi, Ryutaro, Tatsumi, Daisuke, Tsunesada, Yoshiki, Zhu, Zong-Hong, Akutsu, Tomomi, Akutsu, Tomotada, Araya, Akito, Asada, Hideki, Barton, Mark A., Fujiki, Youhei, Fujimoto, Masa-Katsu, Fujita, Ryuichi, Fukushima, Mitsuhiro, Futamase, Toshifumi, Hamuro, Yusaku, Haruyama, Tomiyoshi, Hayakawa, Hideaki, Heinzel, Gerhard, Horikoshi, Gen'ichi, Iguchi, Hideo, Ioka, Kunihito, Ishitsuka, Hideki, Kamikubota, Norihiko, Kaneyama, Takaharu, Karasawa, Yoshikazu, Kasahara, Kunihiko, Kasai, Taketoshi, Katsuki, Mayu, Kawabe, Keita, Kawamura, Mari, Kawashima, Nobuki, Kawazoe, Fumiko, Kokeyama, Keiko, Kozai, Yoshihide, Kudoh, Hideaki, Kuroda, Kazuaki, Kuwabara, Takashi, Matsuda, Namio, Miura, Kazuyuki, Miyakawa, Osamu, Miyama, Shoken, Mizusawa, Hiromi, Musha, Mitsuru, Nagayama, Yoshitaka, Nakagawa, Ken'ichi, Nakamura, Takashi, Nakano, Hiroyuki, Nakao, Ken-ichi, Nishi, Yuhiko, Ogawa, Yujiro, Ohashi, Masatake, Ohishi, Naoko, Okutomi, Akira, Oohara, Ken-ichi, Otsuka, Shigemi, Saito, Yoshio, Sakata, Shihori, Sasaki, Misao, Sato, Kouichi, Sato, Nobuaki, Sato, Youhei, Seki, Hidetsugu, Sekido, Aya, Seto, Naoki, Shibata, Masaru, Shinkai, Hisaaki, Shintomi, Takakazu, Soida, Kenji, Suzuki, Toshikazu, Takamori, Akiteru, Takemoto, Shuzo, Takeno, Kohei, Tanaka, Takahiro, Taniguchi, Keisuke, Taniguchi, Shinsuke, Tanji, Toru, Taylor, C. T., Telada, Souichi, Tochikubo, Kuniharu, Tokunari, Masao, Tomaru, Takayuki, Tsubono, Kimio, Tsuda, Nobuhiro, Uchiyama, Takashi, Ueda, Akitoshi, Ueda, Ken-ichi, Usui, Fumihiko, Waseda, Koichi, Watanabe, Yuko, Yakura, Hiromi, Yamamoto, Akira, Yamamoto, Kazuhiro, Yamazaki, Toshitaka, Ando, Masaki, Kojima, Yasufumi, Arai, Koji, Aso, Youichi, Beyersdorf, Peter, Hayama, Kazuhiro, Iida, Yukiyoshi, Kanda, Nobuyuki, Kawamura, Seiji, Kondo, Kazuhiro, Mio, Norikatsu, Miyoki, Shinji, Moriwaki, Shigenori, Nagano, Shigeo, Numata, Kenji, Sato, Shuichi, Somiya, Kentaro, Tagoshi, Hideyuki, Takahashi, Hirotaka, Takahashi, Ryutaro, Tatsumi, Daisuke, Tsunesada, Yoshiki, Zhu, Zong-Hong, Akutsu, Tomomi, Akutsu, Tomotada, Araya, Akito, Asada, Hideki, Barton, Mark A., Fujiki, Youhei, Fujimoto, Masa-Katsu, Fujita, Ryuichi, Fukushima, Mitsuhiro, Futamase, Toshifumi, Hamuro, Yusaku, Haruyama, Tomiyoshi, Hayakawa, Hideaki, Heinzel, Gerhard, Horikoshi, Gen'ichi, Iguchi, Hideo, Ioka, Kunihito, Ishitsuka, Hideki, Kamikubota, Norihiko, Kaneyama, Takaharu, Karasawa, Yoshikazu, Kasahara, Kunihiko, Kasai, Taketoshi, Katsuki, Mayu, Kawabe, Keita, Kawamura, Mari, Kawashima, Nobuki, Kawazoe, Fumiko, Kokeyama, Keiko, Kozai, Yoshihide, Kudoh, Hideaki, Kuroda, Kazuaki, Kuwabara, Takashi, Matsuda, Namio, Miura, Kazuyuki, Miyakawa, Osamu, Miyama, Shoken, Mizusawa, Hiromi, Musha, Mitsuru, Nagayama, Yoshitaka, Nakagawa, Ken'ichi, Nakamura, Takashi, Nakano, Hiroyuki, Nakao, Ken-ichi, Nishi, Yuhiko, Ogawa, Yujiro, Ohashi, Masatake, Ohishi, Naoko, Okutomi, Akira, Oohara, Ken-ichi, Otsuka, Shigemi, Saito, Yoshio, Sakata, Shihori, Sasaki, Misao, Sato, Kouichi, Sato, Nobuaki, Sato, Youhei, Seki, Hidetsugu, Sekido, Aya, Seto, Naoki, Shibata, Masaru, Shinkai, Hisaaki, Shintomi, Takakazu, Soida, Kenji, Suzuki, Toshikazu, Takamori, Akiteru, Takemoto, Shuzo, Takeno, Kohei, Tanaka, Takahiro, Taniguchi, Keisuke, Taniguchi, Shinsuke, Tanji, Toru, Taylor, C. T., Telada, Souichi, Tochikubo, Kuniharu, Tokunari, Masao, Tomaru, Takayuki, Tsubono, Kimio, Tsuda, Nobuhiro, Uchiyama, Takashi, Ueda, Akitoshi, Ueda, Ken-ichi, Usui, Fumihiko, Waseda, Koichi, Watanabe, Yuko, Yakura, Hiromi, Yamamoto, Akira, Yamamoto, Kazuhiro, and Yamazaki, Toshitaka

Abstract

We present data-analysis schemes and results of observations with the TAMA300 gravitational wave detector, targeting burst signals from stellar-core collapse events. In analyses for burst gravitational waves, the detection and fake-reduction schemes are different from well-investigated ones for a chirp wave analysis, because precise waveform templates are not available. We used an excess -power filter for the extraction of gravitational wave candidates, and developed two methods for the reduction of fake events caused by nonstationary noises of the detector. These analysis schemes were applied to real data from the TAMA300 interferometric gravitational wave detector. As a result, fake events were reduced by a factor of about 1000 in the best cases. In addition, in order to interpret the event candidates from an astronomical viewpoint, we performed a Monte-Carlo simulation with an assumed Galactic event distribution model and with burst waveforms obtained from numerical simulations of stellar-core collapses. We set an upper limit of 5.0×103 events/sec on the burst gravitational wave event rate in our Galaxy with a confidence level of 90%. This work shows prospects on the search for burst gravitational waves, by establishing an analysis scheme for the observation data from an interferometric gravitational wave detector.

Published
2005

2. Comparison of post-Newtonian templates for extreme mass ratio inspirais.

Author

Varma, Vijay, Fujita, Ryuichi, Choudhary, Ashok, and Iyer, Bala R.

Subjects
*NEWTONIAN cosmology, *SUPERMASSIVE stars, *SCHWARZSCHILD black holes, *PARAMETER estimation, *BINARY systems (Astronomy), *LISA Pathfinder
Abstract

Extreme mass ratio inspirais (EMRIs), the inspirais of compact objects into supermassive black holes, are important gravitational wave sources for the Laser Interferometer Space Antenna (LISA). We study the performance of various post-Newtonian (PN) template families relative to the waveforms that are high-precision numerical solutions of the Teukolsky equation in the context of EMRI parameter estimation with LISA. Expressions for the time-domain waveforms TaylorTl, TaylorT2, TaylorT3, TaylorT4 and TaylorEt are derived up to 22 PN order, i.e. O(ν44) (v is the characteristic velocity of the binary) beyond the Newtonian term, for a test particle in a circular orbit around a Schwarzschild black hole. The phase difference between the above 22 PN waveform families and numerical waveforms are evaluated during two-year inspirais for two prototypical EMRI systems with mass ratios 10-4 and 10-5. We find that the déphasés (in radians) for TaylorTl and TaylorT2, respectively, are about 10-9 (10-2) and 10-9 (10-3) for mass ratio 10-4 (10-5). This suggests that using 22 PN TaylorTl or TaylorT2 waveforms for parameter estimation of EMRIs will result in accuracies comparable to numerical waveform accuracy for most of the LISA parameter space. On the other hand, from the dephase results, we find that TaylorT3, TaylorT4 and TaylorEt fare relatively poorly as one approaches the last stable orbit. This implies that, as for comparable mass binaries using the 3.5 PN phase of waveforms, the 22 PN TaylorT3 and TaylorEt approximants do not perform well enough for the EMRIs. The reason underlying the poor performance of TaylorT3, TaylorT4 and TaylorEt relative to TaylorTl and TaylorT2 is finally examined. [ABSTRACT FROM AUTHOR]

Published
2013
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3. Impact of the second-order self-forces on the dephasing of the gravitational waves from quasicircular extreme mass-ratio inspirals.

Author

Isoyama, Soichiro, Fujita, Ryuichi, Sago, Norichika, Tagoshi, Hideyuki, and Tanaka, Takahiro

Subjects
*GRAVITATIONAL waves, *KERR black holes, *BLACK holes, *FLUX (Energy), *PHYSICAL sciences
Abstract

The accurate calculation of the long-term phase evolution of gravitational wave (GW) forms from extreme (intermediate) mass-ratio inspirals [E(I)MRIs] is an inevitable step to extract information from this system. In order to achieve this goal, it is believed that we need to understand the gravitational self- forces. However, it has not been quantitatively demonstrated that the second-order self-forces are necessary for this purpose. In this paper, we revisit the problem to estimate the order of magnitude of the dephasing caused by the second-order self-forces on a small body in a quasicircular orbit around a Kerr black hole, based on the knowledge of the post-Newtonian (PN) approximation and invoking the energy balance argument. In particular, we focus on the averaged dissipative part of the self-force, since it gives the leading-order contribution among their various components. To avoid the possibility of the energy flux of GWs becoming negative, we propose a new simple resummation called exponential resummation, which assures the positivity of the energy flux. In order to estimate the magnitude of the yet-unknown second-order self-forces, here we point out the scaling property in the absolute value of the PN coefficients of the energy flux. Using these new tools, we evaluate the expected magnitude of dephasing. Our analysis indicates that the dephasing due to the second-order self-forces for quasicircular E(I)MRIs may be well captured by the 3 PN energy flux, once we obtain all the spin-dependent terms, except for the case with an extremely large spin of the central Kerr black hole. [ABSTRACT FROM AUTHOR]

Published
2013
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4. Observation results by the TAMA300 detector on gravitational wave bursts from stellar-core collapses

Author

Ando, Masaki, Kojima, Yasufumi, Arai, Koji, Aso, Youichi, Beyersdorf, Peter, Hayama, Kazuhiro, Iida, Yukiyoshi, Kanda, Nobuyuki, Kawamura, Seiji, Kondo, Kazuhiro, Mio, Norikatsu, Miyoki, Shinji, Moriwaki, Shigenori, Nagano, Shigeo, Numata, Kenji, Sato, Shuichi, Somiya, Kentaro, Tagoshi, Hideyuki, Takahashi, Hirotaka, Takahashi, Ryutaro, Tatsumi, Daisuke, Tsunesada, Yoshiki, Zhu, Zong-Hong, Akutsu, Tomomi, Akutsu, Tomotada, Araya, Akito, Asada, Hideki, Barton, Mark A., Fujiki, Youhei, Fujimoto, Masa-Katsu, Fujita, Ryuichi, Fukushima, Mitsuhiro, Futamase, Toshifumi, Hamuro, Yusaku, Haruyama, Tomiyoshi, Hayakawa, Hideaki, Heinzel, Gerhard, Horikoshi, Gen'ichi, Iguchi, Hideo, Ioka, Kunihito, Ishitsuka, Hideki, Kamikubota, Norihiko, Kaneyama, Takaharu, Karasawa, Yoshikazu, Kasahara, Kunihiko, Kasai, Taketoshi, Katsuki, Mayu, Kawabe, Keita, Kawamura, Mari, Kawashima, Nobuki, Kawazoe, Fumiko, Kokeyama, Keiko, Kozai, Yoshihide, Kudoh, Hideaki, Kuroda, Kazuaki, Kuwabara, Takashi, Matsuda, Namio, Miura, Kazuyuki, Miyakawa, Osamu, Miyama, Shoken, Mizusawa, Hiromi, Musha, Mitsuru, Nagayama, Yoshitaka, Nakagawa, Ken'ichi, Nakamura, Takashi, Nakano, Hiroyuki, Nakao, Ken-ichi, Nishi, Yuhiko, Ogawa, Yujiro, Ohashi, Masatake, Ohishi, Naoko, Okutomi, Akira, Oohara, Ken-ichi, Otsuka, Shigemi, Saito, Yoshio, Sakata, Shihori, Sasaki, Misao, Sato, Kouichi, Sato, Nobuaki, Sato, Youhei, Seki, Hidetsugu, Sekido, Aya, Seto, Naoki, Shibata, Masaru, Shinkai, Hisaaki, Shintomi, Takakazu, Soida, Kenji, Suzuki, Toshikazu, Takamori, Akiteru, Takemoto, Shuzo, Takeno, Kohei, Tanaka, Takahiro, Taniguchi, Keisuke, Taniguchi, Shinsuke, Tanji, Toru, Taylor, C. T., Telada, Souichi, Tochikubo, Kuniharu, Tokunari, Masao, Tomaru, Takayuki, Tsubono, Kimio, Tsuda, Nobuhiro, Uchiyama, Takashi, Ueda, Akitoshi, Ueda, Ken-ichi, Usui, Fumihiko, Waseda, Koichi, Watanabe, Yuko, Yakura, Hiromi, Yamamoto, Akira, Yamamoto, Kazuhiro, Yamazaki, Toshitaka, Ando, Masaki, Kojima, Yasufumi, Arai, Koji, Aso, Youichi, Beyersdorf, Peter, Hayama, Kazuhiro, Iida, Yukiyoshi, Kanda, Nobuyuki, Kawamura, Seiji, Kondo, Kazuhiro, Mio, Norikatsu, Miyoki, Shinji, Moriwaki, Shigenori, Nagano, Shigeo, Numata, Kenji, Sato, Shuichi, Somiya, Kentaro, Tagoshi, Hideyuki, Takahashi, Hirotaka, Takahashi, Ryutaro, Tatsumi, Daisuke, Tsunesada, Yoshiki, Zhu, Zong-Hong, Akutsu, Tomomi, Akutsu, Tomotada, Araya, Akito, Asada, Hideki, Barton, Mark A., Fujiki, Youhei, Fujimoto, Masa-Katsu, Fujita, Ryuichi, Fukushima, Mitsuhiro, Futamase, Toshifumi, Hamuro, Yusaku, Haruyama, Tomiyoshi, Hayakawa, Hideaki, Heinzel, Gerhard, Horikoshi, Gen'ichi, Iguchi, Hideo, Ioka, Kunihito, Ishitsuka, Hideki, Kamikubota, Norihiko, Kaneyama, Takaharu, Karasawa, Yoshikazu, Kasahara, Kunihiko, Kasai, Taketoshi, Katsuki, Mayu, Kawabe, Keita, Kawamura, Mari, Kawashima, Nobuki, Kawazoe, Fumiko, Kokeyama, Keiko, Kozai, Yoshihide, Kudoh, Hideaki, Kuroda, Kazuaki, Kuwabara, Takashi, Matsuda, Namio, Miura, Kazuyuki, Miyakawa, Osamu, Miyama, Shoken, Mizusawa, Hiromi, Musha, Mitsuru, Nagayama, Yoshitaka, Nakagawa, Ken'ichi, Nakamura, Takashi, Nakano, Hiroyuki, Nakao, Ken-ichi, Nishi, Yuhiko, Ogawa, Yujiro, Ohashi, Masatake, Ohishi, Naoko, Okutomi, Akira, Oohara, Ken-ichi, Otsuka, Shigemi, Saito, Yoshio, Sakata, Shihori, Sasaki, Misao, Sato, Kouichi, Sato, Nobuaki, Sato, Youhei, Seki, Hidetsugu, Sekido, Aya, Seto, Naoki, Shibata, Masaru, Shinkai, Hisaaki, Shintomi, Takakazu, Soida, Kenji, Suzuki, Toshikazu, Takamori, Akiteru, Takemoto, Shuzo, Takeno, Kohei, Tanaka, Takahiro, Taniguchi, Keisuke, Taniguchi, Shinsuke, Tanji, Toru, Taylor, C. T., Telada, Souichi, Tochikubo, Kuniharu, Tokunari, Masao, Tomaru, Takayuki, Tsubono, Kimio, Tsuda, Nobuhiro, Uchiyama, Takashi, Ueda, Akitoshi, Ueda, Ken-ichi, Usui, Fumihiko, Waseda, Koichi, Watanabe, Yuko, Yakura, Hiromi, Yamamoto, Akira, Yamamoto, Kazuhiro, and Yamazaki, Toshitaka

Abstract

We present data-analysis schemes and results of observations with the TAMA300 gravitational wave detector, targeting burst signals from stellar-core collapse events. In analyses for burst gravitational waves, the detection and fake-reduction schemes are different from well-investigated ones for a chirp wave analysis, because precise waveform templates are not available. We used an excess -power filter for the extraction of gravitational wave candidates, and developed two methods for the reduction of fake events caused by nonstationary noises of the detector. These analysis schemes were applied to real data from the TAMA300 interferometric gravitational wave detector. As a result, fake events were reduced by a factor of about 1000 in the best cases. In addition, in order to interpret the event candidates from an astronomical viewpoint, we performed a Monte-Carlo simulation with an assumed Galactic event distribution model and with burst waveforms obtained from numerical simulations of stellar-core collapses. We set an upper limit of 5.0×103 events/sec on the burst gravitational wave event rate in our Galaxy with a confidence level of 90%. This work shows prospects on the search for burst gravitational waves, by establishing an analysis scheme for the observation data from an interferometric gravitational wave detector.

5. Ultralight scalars and resonances in black-hole physics.

Author

Fujita, Ryuichi and Cardoso, Vitor

Subjects
*RESONANCE, *BLACK holes
Abstract

Ultralight degrees of freedom coupled to matter lead to resonances, which can be excited when the Compton wavelength of the field equals a dynamical scale in the problem. For binaries composed of a star orbiting a supermassive black hole, these resonances lead to a smoking-gun effect: a periastron distance which stalls, even in the presence of gravitational-wave dissipation. This effect, also called a floating orbit, occurs for generic equatorial but eccentric orbits, and we argue that finite-size effects are not enough to suppress it. [ABSTRACT FROM AUTHOR]

Published
2017
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6. Post-Newtonian factorized multipolar waveforms for spinning, nonprecessing black-hole binaries.

Author

Yi Pan, Buonanno, Alessandra, Fujita, Ryuichi, Racine, Etienne, and Tagoshi, Hideyuki

Subjects
*NEWTONIAN cosmology, *METAPHYSICAL cosmology, *BLACK holes, *COMPACT objects (Astronomy), *BINARY stars
Abstract

We generalize the factorized resummation of multipolar waveforms introduced by Damour, Iyer, and Nagar to spinning black holes. For a nonspinning test particle spiraling a Kerr black hole in the equatorial plane, we find that factorized multipolar amplitudes which replace the residual relativistic amplitude fℓm with its ℓth root, ρℓm=fℓm1/ℓ, agree quite well with the numerical amplitudes up to the Kerr-spin value q≤0.95 for orbital velocities v≤0.4. The numerical amplitudes are computed solving the Teukolsky equation with a spectral code. The agreement for prograde orbits and large spin values of the Kerr black-hole can be further improved at high velocities by properly factoring out the lower-order post-Newtonian contributions in ρℓm. The resummation procedure results in a better and systematic agreement between numerical and analytical amplitudes (and energy fluxes) than standard Taylor-expanded post-Newtonian approximants. This is particularly true for higher-order modes, such as (2,1), (3,3), (3,2), and (4,4), for which less spin post-Newtonian terms are known. We also extend the factorized resummation of multipolar amplitudes to generic mass-ratio, nonprecessing, spinning black holes. Lastly, in our study we employ new, recently computed, higher-order post-Newtonian terms in several subdominant modes and compute explicit expressions for the half and one-and-half post-Newtonian contributions to the odd-parity (current) and even-parity (odd) multipoles, respectively. Those results can be used to build more accurate templates for ground-based and space-based gravitational-wave detectors. [ABSTRACT FROM AUTHOR]

Published
2011
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7. Adiabatic Waveforms from Extreme-Mass-Ratio Inspirals: An Analytical Approach.

Author

Isoyama S, Fujita R, Chua AJK, Nakano H, Pound A, and Sago N

Abstract

Scientific analysis for the gravitational wave detector LISA will require theoretical waveforms from extreme-mass-ratio inspirals (EMRIs) that extensively cover all possible orbital and spin configurations around astrophysical Kerr black holes. However, on-the-fly calculations of these waveforms have not yet overcome the high dimensionality of the parameter space. To confront this challenge, we present a user-ready EMRI waveform model for generic (eccentric and inclined) orbits in Kerr spacetime, using an analytical self-force approach. Our model accurately covers all EMRIs with arbitrary inclination and black hole spin, up to modest eccentricity (≲0.3) and separation (≳2-10  M from the last stable orbit). In that regime, our waveforms are accurate at the leading "adiabatic" order, and they approximately capture transient self-force resonances that significantly impact the gravitational wave phase. The model fills an urgent need for extensive waveforms in ongoing data-analysis studies, and its individual components will continue to be useful in future science-adequate waveforms.

Published
2022
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