Kohei Inayoshi
Columbia University
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Featured researches published by Kohei Inayoshi.
The Astrophysical Journal | 2013
Takashi Hosokawa; Harold W. Yorke; Kohei Inayoshi; Kazuyuki Omukai; Naoki Yoshida
Supermassive stars (SMSs) forming via very rapid mass accretion (Mdot >~ 0.1 Msun/yr) could be precursors of supermassive black holes observed beyond redshift of about 6. Extending our previous work, we here study the evolution of primordial stars growing under such rapid mass accretion until the stellar mass reaches 10^{4 - 5} Msun. Our stellar evolution calculations show that a star becomes supermassive while passing through the supergiant protostar stage, whereby the star has a very bloated envelope and a contracting inner core. The stellar radius increases monotonically with the stellar mass, until =~ 100 AU for M_* >~ 10^4 Msun, after which the star begins to slowly contract. Because of the large radius the effective temperature is always less than 10^4 K during rapid accretion. The accreting material is thus almost completely transparent to the stellar radiation. Only for M_* >~ 10^5 Msun can stellar UV feedback operate and disturb the mass accretion flow. We also examine the pulsation stability of accreting SMSs, showing that the pulsation-driven mass loss does not prevent stellar mass growth. Observational signatures of bloated SMSs should be detectable with future observational facilities such as the James Webb Space Telescope. Our results predict that an inner core of the accreting SMS should suffer from the general relativistic instability soon after the stellar mass exceeds 10^5 Msun. An extremely massive black hole should form after the collapse of the inner core.
Monthly Notices of the Royal Astronomical Society | 2014
Tomoya Kinugawa; Kohei Inayoshi; Kenta Hotokezaka; Daisuke Nakauchi; Takashi Nakamura
We perform population synthesis simulations for Population III (Pop III) coalescing binary neutron stars (NS-NSs), neutron star - black hole binaries (NS-BHs), and binary black holes (BH-BHs) which merge within the age of the universe. We found that the typical mass of Pop III BH-BHs is
Monthly Notices of the Royal Astronomical Society | 2012
Kohei Inayoshi; Kazuyuki Omukai
sim 30 rm{M}_{odot}
Monthly Notices of the Royal Astronomical Society | 2016
Kohei Inayoshi; Zoltan Haiman; Jeremiah P. Ostriker
so that the inspiral chirp signal of gravitational waves can be detected up to z=0.28 by KAGRA, Adv. LIGO, Adv. Virgo and GEO network. Our simulations suggest that the detection rate of the coalescing Pop III BH-BHs is
Monthly Notices of the Royal Astronomical Society | 2014
Kohei Inayoshi; Kazuyuki Omukai; Elizabeth J. Tasker
140 (68) cdot ({rm SFR}_{rm p}/10^{-2.5} rm{M}_{odot} {rm yr}^{-1} {rm Mpc}^{-3}) cdot {rm Err}_{rm sys} ~{rm events} ~{rm yr}^{-1}
Monthly Notices of the Royal Astronomical Society | 2015
Kohei Inayoshi; Takamitsu Tanaka
for the flat (Salpeter) initial mass function (IMF), respectively, where
Monthly Notices of the Royal Astronomical Society | 2011
Kohei Inayoshi; Kazuyuki Omukai
rm SFR_p
Monthly Notices of the Royal Astronomical Society | 2014
Kohei Inayoshi; Zoltan Haiman
and
Monthly Notices of the Royal Astronomical Society | 2016
Kohei Inayoshi; Kazumi Kashiyama; Eli Visbal; Zoltan Haiman
rm Err_{sys}
Monthly Notices of the Royal Astronomical Society | 2015
Kohei Inayoshi; Eli Visbal; Kazumi Kashiyama
are the peak value of the Pop III star formation rate and the possible systematic errors due to the assumptions in Pop III population synthesis, respectively.