AMAkira Mizuno

Akira Mizuno

*This is an algorithmically generated author record based on publicly available information.

Current Organizations / Institutes

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Previous Organizations / Institutes

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Akira Mizuno has a total of 178 co-authors. Here are the top co-authors by number of shared publications:

  • Yasuo Fukui

    Department of Astrophysics Nagoya University 464-8602 Furocho Chikusaku Nagoya Japan

    11 shared publications
  • Toshikazu Onishi

    Department of Astrophysics, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602 y

    10 shared publications
  • Yasuo Fukui

    Department of Physics, Nagoya University , Furo-cho, Chikusa-ku, Nagoya, Aichi 464-8601

    9 shared publications
  • Akiko Kawamura

    Department of Astrophysics, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602 y

    8 shared publications
  • Hideo Ogawa

    Department of Astrophysics, Nagoya University, Chikusa-ku, Nagoya 464-8602

    8 shared publications
  • Norikazu Mizuno

    Department of Astrophysics, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602 y

    8 shared publications

Latest Publications

  • 4362Effect of intravenous carperitide versus nitrates as first-line vasodilators on in-hospital outcomes in hospitalized patients with acute heart failure: insight from a nationwide claim-based database

    by T Nagai, N Iwakami, M Nakai, K Nishimura, Y Sumita, A Mizuno, H Tsutsui, H Ogawa, T Anzai, the JROAD Study Group

    Background: Carperitide (CAR) is a recombinantly produced intravenous formulation of human atrial natriuretic peptide. Despite of negative impacts of nesiritide on clinical outcomes for acute heart failure (AHF), CAR has been used for around a half of Japanese AHF patients as a vasodilator based on limited evidences.

  • Star Forming Dense Cloud Cores in the TeV -ray SNR RX J1713.7-3946

    by Sano Hidetoshi, H. Sano, J. Sato, H. Yamamoto, T. Hayakawa, K. Torii, N. Moribe, A. Kawamura, T. Okuda, N. Mizuno, et al.

    RX J1713.7-3946 is one of the TeV {gamma}-ray supernova remnants (SNRs) emitting synchrotron X rays. The SNR is associated with molecular gas located at {approx}1 kpc. We made new molecular observations toward the dense cloud cores, peaks A, C and D, in the SNR in the {sup 12}CO(J=2-1) and {sup 13}CO(J=2-1) transitions at angular resolution of 90 degrees. The most intense core in {sup 13}CO, peak C, was also mapped in the {sup 12}CO(J=4-3) transition at angular resolution of 38 degrees. Peak C shows strong signs of active star formation including bipolar outflow and a far-infrared protostellar source and has a steep gradient with a r{sup -2.2 {+-} 0.4} variation in the average density within radius r. Peak C and the other dense cloud cores are rim-brightened in synchrotron X rays, suggesting that the dense cloud cores are embedded within or on the outer boundary of the SNR shell. This confirms the earlier suggestion that the X rays are physically associated with the molecular gas (Fukui et al. 2003). We present a scenario where the densest molecular core, peak C, survived against the blast wave and is now embedded within the SNR. Numerical simulations of the shock-cloud interaction indicate thatmore » a dense clump can indeed survive shock erosion, since shock propagation speed is stalled in the dense clump. Additionally, the shock-cloud interaction induces turbulence and magnetic field amplification around the dense clump that may facilitate particle acceleration in the lower-density inter-clump space leading to the enhanced synchrotron X rays around dense cores. « less

  • Open Access

    Warm and Dense Molecular Gas in the N 159 Region: 12CO J = 4–3 and 13CO J = 3–2 Observations with NANTEN2 and ASTE

    by Yoji Mizuno, Akiko Kawamura, Toshikazu Onishi, Tetsuhiro Minamidani, Erik Muller, Hiroaki Yamamoto, Takahiro Hayakawa, Norikazu Mizuno, Akira Mizuno, Jürgen Stutzki, et al.

    New $$^{12}$$CO $$J =$$ 4–3 and $$^{13}$$CO $$J =$$ 3–2 observations of the N 159 region, an active site of massive star formation in the Large Magellanic Cloud, have been made with the NANTEN2 and ASTE submillimeter telescopes, respectively. The $$^{12}$$CO $$J =$$ 4–3 distribution is separated into three clumps, each associated with N 159 W, N 159 E, and N 159 S. These new measurements toward the three clumps are used in coupled calculations of molecular rotational excitation and line radiation transfer, along with other transitions of the $$^{12}$$CO $$J =$$ 1–0, $$J =$$ 2–1, $$J =$$ 3–2, and $$J =$$ 7–6 as well as the isotope transitions of $$^{13}$$CO $$J =$$ 1–0, $$J =$$ 2–1, $$J =$$ 3–2, and $$J =$$ 4–3. The $$^{13}$$CO $$J =$$ 3–2 data were newly taken for the present work. The temperatures and densities were found to be $$\sim$$70&x2013;80 K and $$\sim$$3 $$\times$$ 10$$^{3}$$cm$$^{-3}$$ in N 159 W and N 159 E, and $$\sim$$30 K and $$\sim$$1.6 $$\times$$ 10$$^{3}$$cm$$^{-3}$$ in N 159 S. These results were compared with the star-formation activity based on data of young stellar clusters and HII regions as well as midinfrared emission obtained with the Spitzer MIPS. The N 159 E clump is associated with cluster(s) embedded, as observed at 24$$\mu$$m by the Spitzer MIPS, and the derived high temperature, 80 K, is interpreted as being heated by these sources. The N 159 E clump is likely to be responsible for a dark lane in a large H II region by dust extinction. On the other hand, the N 159 W clump is associated with clusters embedded mainly toward the eastern edge of the clump only. These clusters show offsets of 20$${}^{\prime\prime}$$–40$${}^{\prime\prime}$$ from the $$^{12}$$CO $$J =$$ 4–3 peak, and are probably responsible for heating indicated by the derived high temperature, 70 K. The N 159 W clump exhibits no sign of star formation toward the $$^{12}$$CO $$J =$$ 4–3 peak position and its western region that shows enhanced $$R_{4-3/1-0}$$ and $$R_{3-2/1-0}$$ ratios. We therefore suggest that the N 159 W peak represents a pre-star-cluster core of $$\sim$$10$$^{5} M_{\odot}$$ which deserves further detailed studies. The N 159 S clump shows little sign of star formation, as is consistent with the lower temperature, 30 K, and has a somewhat lower density than N 159 W and N 159 E. The N 159 S clump is also a candidate for future star formation.


  • Open Access

    Warm and Dense Molecular Gas in the N159 Region: 12CO J=4-3 and 13CO J=3-2 Observations with NANTEN2 and ASTE

    by Yoji Mizuno, Akiko Kawamura, Toshikazu Onishi, Tetsuhiro Minamidani, Erik Muller, Hiroaki Yamamoto, Takahiro Hayakawa, Norikazu Mizuno, Akira Mizuno, Jurgen Stutzki, et al.

    New 12CO J=4-3 and 13CO J=3-2 observations of the N159 region in the Large Magellanic Cloud have been made. The 12CO J=4-3 distribution is separated into three clumps. These new measurements toward the three clumps are used in coupled calculations of molecular rotational excitation and line radiation transfer, along with other transitions of the 12CO as well as the isotope transitions of 13CO. The temperatures and densities are determined to be ~70-80K and ~3x10^3 cm-3 in N159W and N159E and ~30K and ~1.6x10^3 cm-3 in N159S. These results are compared with the star formation activity. The N159E clump is associated with embedded cluster(s) as observed at 24 micron and the derived high temperature is explained as due to the heating by these sources. The N159E clump is likely responsible for a dark lane in a large HII region by the dust extinction. The N159W clump is associated with embedded clusters mainly toward the eastern edge of the clump only. These clusters show offsets of 20"-40" from the 12CO J=4-3 peak and are probably responsible for heating indicated by the derived high temperature. The N159W clump exhibits no sign of star formation toward the 12CO J=4-3 peak position and its western region. We suggest that the N159W peak represents a pre-star-cluster core of ~105M_sol which deserves further detailed studies. Note that recent star formation took place between N159W and N159E as indicated by several star clusters and HII regions, while the natal molecular gas toward the stars have already been dissipated by the ionization and stellar winds of the OB stars. The N159S clump shows little sign of star formation as is consistent with the lower temperature and somewhat lower density. The N159S clump is also a candidate for future star formation.

  • SPITZERSAGE SURVEY OF THE LARGE MAGELLANIC CLOUD. III. STAR FORMATION AND ∼1000 NEW CANDIDATE YOUNG STELLAR OBJECTS

    by B. A. Whitney, M. Sewilo, R. Indebetouw, T. P. Robitaille, M. Meixner, K. Gordon, M. R. Meade, B. L. Babler, J. Harris, J. L. Hora, et al.


  • Open Access

    Spitzer Survey of the Large Magellanic Cloud, Surveying the Agents of a Galaxy's Evolution (SAGE) I: Overview and Initial Results

    by Margaret Meixner, Karl D. Gordon, Remy Indebetouw, Joseph L. Hora, Barbara Whitney, Robert Blum, William Reach, Jean-Philippe Bernard, Marilyn Meade, Brian Babler, et al.

    We are performing a uniform and unbiased, ~7x7 degrees imaging survey of the Large Magellanic Cloud (LMC), using the IRAC and MIPS instruments on board the Spitzer Space Telescope in order to survey the agents of a galaxy's evolution (SAGE), the interstellar medium (ISM) and stars in the LMC. The detection of diffuse ISM with column densities >1.2x10^21 H cm^-2 permits detailed studies of dust processes in the ISM. SAGE's point source sensitivity enables a complete census of newly formed stars with masses >3 solar masses that will determine the current star formation rate in the LMC. SAGE's detection of evolved stars with mass loss rates >1x10^-8 solar masses per year will quantify the rate at which evolved stars inject mass into the ISM of the LMC. The observing strategy includes two epochs in 2005, separated by three months, that both mitigate instrumental artifacts and constrain source variability. The SAGE data are non-proprietary. The data processing includes IRAC and MIPS pipelines and a database for mining the point source catalogs, which will be released to the community in support of Spitzer proposal cycles 4 and 5. We present initial results on the epoch 1 data with a special focus on the N79 and N83 region. The SAGE epoch 1 point source catalog has ~4 million sources. The point source counts are highest for the IRAC 3.6 microns band and decrease dramatically towards longer wavelengths consistent with the fact that stars dominate the point source catalogs and that the dusty objects, e.g. young stellar objects and dusty evolved stars that detected at the longer wavelengths, are rare in comparison. We outline a strategy for identifying foreground MW stars, that may comprise as much as 18% of the source list, and background galaxies, that may comprise ~12% of the source list.

  • Top Cited Papers
    Open Access

    SpitzerSurvey of the Large Magellanic Cloud: Surveying the Agents of a Galaxy?s Evolution (SAGE). I. Overview and Initial Results

    by Margaret Meixner, Karl D. Gordon, Remy Indebetouw, Joseph L. Hora, Barbara Whitney, Robert Blum, William Reach, Jean‐Philippe Bernard, Marilyn Meade, Brian Babler, et al.


  • High‐Latitude Molecular Clouds in an HiFilament toward the MBM 53, 54, and 55 Complex: Existence of an H2Cloud with Low CO Intensity

    by H. Yamamoto, T. Onishi, A. Mizuno, Y. Fukui

    We carried out a CO survey of high Galactic latitude molecular clouds toward an H I filament that contains a molecular cloud complex, MBM 53, 54, and 55, with the NANTEN telescope. Our observation covered the whole area of the H I filament in 12CO (J = 1-0) with a 4' grid spacing. The filament is found to consist of a number of clumpy molecular clouds, and we identified 110 12CO clouds in the region, whose total mass is estimated to be ~1200 M☉. 13CO (J = 1-0) observations were carried out toward the region of high 12CO intensities in order to measure the optical depth of molecular gas. There is no detection in C18O (J = 1-0) line in the observed region, indicating that there are no clouds dense enough to form stars in the near future. These observations spatially resolved the entire gas distribution of MBM 53, 54, and 55 for the first time, and we have found a massive cloud, HLCG 92-35, around (l, b) ~ (92°, -35°) whose mass is ~330 M☉, corresponding to ~1/4 of the total mass. This CO cloud occupies the Galactic western half of a circular H I cloud toward (l, b) = (935, -355), and the H I to CO mass ratio is estimated to be the largest in the observed region. The far-infrared excess over H I emission, which is a good indicator of an existence of molecular hydrogen, toward HLCG 92-35 is the largest in the observed region. The ratio of the luminosity of the infrared excess to CO mass is also significantly larger than those of the other clouds, by a factor of ~5. These facts indicate that HLCG 92-35 is a CO-forming molecular cloud, which is younger than the MBM clouds in terms of molecular cloud formation. Some past explosive event has been suggested toward the H I filament. Toward HLCG 92-35, the molecular gas distributed along the western edge of the H I cloud, which implies that the molecular gas may be formed by a compression of expanding H I shell.


  • Open Access

    Statistical study of C$\mathsf{^{18}}$O dense cloud cores and star formation

    by K. Tachihara, T. Onishi, A. Mizuno, Y. Fukui

    Astronomy & Astrophysics (A&A) is an international journal which publishes papers on all aspects of astronomy and astrophysics


  • Open Access

    On the Mass Spectrum of Giant Molecular Clouds in the Large Magellanic Cloud

    by Yasuo Fukui, Norikazu Mizuno, Reiko Yamaguchi, Akira Mizuno, Toshikazu Onishi

    Based on a new sensitive survey of the giant molecular clouds (GMCs) in the Large Magellanic Cloud, we derived the mass spectrum for them. In the mass range from $\sim8\times10^4\,{{{M}_{\odot}}}$ to $3\times10^6\,{{{M}_{\odot}}}$, a power law with an index value of $-1.9\pm0.1$ shows the best fit to the data. This is consistent with numerical simulations that explain both the H i and CO clumpy distributions by Wada et al. (2000; ApJ, 540, 797), but is significantly steeper than that of the GMCs in the Galaxy. This may be consistent with the drastic dissipation of the GMCs in the LMC due to higher UV radiation fields than in the Galaxy.