29 research outputs found

    Neutrino emissions in all flavors up to the pre-bounce of massive stars and the possibility of their detections

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    This paper is a sequel to our previous one (Kato et al.2015), which calculated the luminosities and spectra of electron-type anti-neutrinos (νˉe\bar{\nu}_e's) from the progenitors of core-collapse supernovae. Expecting that a capability to detect electron-type neutrinos (νe\nu_e's) will increase dramatically with the emergence of liquid-argon detectors such as DUNE, we broaden the scope in this study to include all-flavors of neutrinos emitted from the pre-bounce phase. We pick up three progenitor models of an electron capture supernova (ECSN) and iron-core collapse supernovae (FeCCSNe). We find that the number luminosities reach ∼1057s−1\sim10^{57} \mathrm{s^{-1}} and ∼1053s−1\sim10^{53} \mathrm{s^{-1}} at maximum for νe\nu_e and νˉe\bar{\nu}_e, respectively. We also estimate the numbers of detection events at terrestrial neutrino detectors including DUNE, taking flavor oscillations into account and assuming the distance to the progenitors to be 200 pc. It is demonstrated that νˉe\bar{\nu}_e's from the ECSN-progenitor will be undetected at almost all detectors, whereas we will be able to observe ≳\gtrsim15900 νe\nu_e's at DUNE for the inverted mass hierarchy. From the FeCCSN-progenitors, the number of νˉe\bar{\nu}_e events will be largest for JUNO, 200-900 νˉe\bar{\nu}_e's, depending on the mass hierarchy whereas the number of νe\nu_e events at DUNE is ≳\gtrsim2100 for the inverted mass hierarchy. These results imply that the detection of νˉe\bar{\nu}_e's is useful to distinguish FeCCSN- from ECSN-progenitors, while νe\nu_e's will provide us with detailed information on the collapse phase regardless of the type and mass of progenitor.Comment: 22 pages, 14 figures, 4 tables, accepted to Ap

    Pulsational Pair-instability Supernovae. II. Neutrino Signals from Pulsations and Their Detection by Terrestrial Neutrino Detectors

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    A Pulsational Pair-instability supernova (PPISN) evolves from a massive star with a mass ~80–140 M⊙ that develops electron–positron pair-instability after hydrostatic He-burning in the core has finished. In Leung et al. (Paper I), we examined the evolutionary tracks and the pulsational mass-loss history of this class of stars. In this paper, we analyze the thermodynamical history to explore the neutrino observables of PPISNe. We compute the neutrino light curves and spectra during pulsation. We then study the detailed neutrino emission profiles of these stars and estimate the expected neutrino detection count for different terrestrial neutrino detectors, including, e.g., KamLAND and Super-Kamiokande. Finally, we compare the neutrino pattern of PPISN with other types of supernovae based on a canonical 10 kt detector. The predicted neutrino signals can provide an early warning for telescopes to trace for the early time optical signals. The implications of neutrino physics on the expected detection are also discussed

    Upper Limit on Gravitational Wave Backgrounds at 0.2 Hz with Torsion-bar Antenna

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    We present the first upper limit on gravitational wave (GW) backgrounds at an unexplored frequency of 0.2 Hz using a torsion-bar antenna (TOBA). A TOBA was proposed to search for low-frequency GWs. We have developed a small-scaled TOBA and successfully found {\Omega}gw(f) < 4.3 \times 1017 at 0.2 Hz as demonstration of the TOBA's capabilities, where {\Omega}gw (f) is the GW energy density per logarithmic frequency interval in units of the closure density. Our result is the first nonintegrated limit to bridge the gap between the LIGO band (around 100 Hz) and the Cassini band (10-6 - 10-4 Hz).Comment: 4 pages, 5 figure
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