研究者業績

山村 一誠

ヤマムラ イッセイ  (Issei Yamamura)

基本情報

所属
国立研究開発法人宇宙航空研究開発機構 宇宙科学研究所 准教授
学位
博士(理学)(1995年3月 東京大学)

J-GLOBAL ID
200901077188018891
researchmap会員ID
1000304542

主要な論文

 114
  • Toshiya Ueta, Rachael L. Tomasino, Satoshi Takita, Hideyuki Izumiura, Mai Shirahata, Andrew Fullard, Issei Yamamura, Shuji Matsuura
    PUBLICATIONS OF THE ASTRONOMICAL SOCIETY OF JAPAN 69(1) 2017年2月  査読有り
    We present a general surface brightness correction method for compact extended sources imaged in the slow-scan pointed observation mode of the Far-Infrared Surveyor (FIS) aboard the AKARI infrared astronomical satellite. Our method recovers correct surface brightness distribution maps by rescaling archived raw FIS maps using the surfacebrightness-dependent inverse FIS response function. The flux of a target source is then automatically corrected for as the simple sum of surface brightnesses within the adopted contour encircling the perimeter of the target (i.e., contour photometry). This correction method is contrasted with the previous aperture photometry method for point sources, which directly corrects for the target flux with a flux-dependent scaling law. The new surface brightness correction scheme is applicable to objects of any shape from unresolved point sources to resolved extended objects, as long as the target is not deemed diffuse, i.e., the total extent of the target source does not exceed too much more than a single FIS scan width of 10. The new correction method takes advantage of the well-defined shape (i.e., the scale invariance) of the point spread function, which enables us to adopt a power-law FIS response function. We analyze the point source photometric calibrator data using the FIS AKARI Slow-scan Tool and constrain the parameters of the adopted power-law FIS response function. We conclude that the photometric accuracy of the new correction method is better than 10% error based on comparisons with the expected fluxes of the photometric calibrators, and that resulting fluxes without the present correction method can lead to up to 230% overestimates or down to 50% underestimates.
  • S. Sorahana, I. Yamamura
    ASTROPHYSICAL JOURNAL 793(1) 2014年9月  査読有り
    The detection of the CO2 absorption band at 4.2 mu(m) in brown dwarf spectra by AKARI has made it possible to discuss CO2 molecular abundance in brown dwarf atmospheres. In our previous studies, we found an excess in the 4.2 mu m CO2 absorption band of three brown dwarf spectra, and suggested that these deviations were caused by high C and O elemental abundances in their atmospheres. To validate this hypothesis, we have constructed a set of models of brown dwarf atmospheres with various elemental abundance patterns, and we investigate the variations of the molecular composition and the thermal structure, and how they affect the near-infrared spectra between 1.0 and 5.0 mu m. The 4.2 mu m CO2 absorption band in some late-L and T dwarfs taken by AKARI is stronger or weaker than predicted by corresponding models with solar abundance. By comparing the CO2 band in the model spectra to the observed near-infrared spectra, we confirm possible elemental abundance variations among brown dwarfs. We find that the band strength is especially sensitive to O abundance, but C is also needed to reproduce the entire near-infrared spectra. This result indicates that both the C and O abundances should increase and decrease simultaneously for brown dwarfs. We find that a weaker CO2 absorption band in a spectrum can also be explained by a model with lower "C and O" abundances.
  • S. Sorahana, I. Yamamura, H. Murakami
    Astrophysical Journal 767(1) 2013年4月10日  査読有り
    We derive the radii of 16 brown dwarfs observed by AKARI using their parallaxes and the ratios of observed to model fluxes. We find that the brown dwarf radius ranges between 0.64-1.13 RJ with an average radius of 0.83 RJ . We find a trend in the relation between radii and T eff the radius is at a minimum at T eff ∼ 1600 K, which corresponds to the spectral types of mid- to late-L. The result is interpreted by a combination of radius-mass and radius-age relations that are theoretically expected for brown dwarfs older than 108 yr. © 2013. The American Astronomical Society. All rights reserved..
  • S. Sorahana, I. Yamamura
    ASTROPHYSICAL JOURNAL 760(2) 2012年12月  査読有り
    We investigate variations in the strengths of three molecular bands, CH4 at 3.3 mu m, CO at 4.6 mu m, and CO2 at 4.2 mu m, in 16 brown dwarf spectra obtained by AKARI. Spectral features are examined along the sequence of source classes from L1 to T8. We find that the CH4 3.3 mu m band is present in the spectra of brown dwarfs later than L5, and the CO 4.6 mu m band appears in all spectral types. The CO2 absorption band at 4.2 mu m is detected in late-L and T-type dwarfs. To better understand brown dwarf atmospheres, we analyze the observed spectra using the Unified Cloudy Model. The physical parameters of the AKARI sample, i.e., atmospheric effective temperature T-eff, surface gravity log g, and critical temperature T-cr, are derived. We also model IRTF/SpeX and UKIRT/CGS4 spectra in addition to the AKARI data in order to derive the most probable physical parameters. Correlations between the spectral type and the modeled parameters are examined. We confirm that the spectral-type sequence of late-L dwarfs is not related to T-eff, but instead originates as a result of the effect of dust.
  • Poshak Gandhi, Issei Yamamura, Satoshi Takita
    ASTROPHYSICAL JOURNAL LETTERS 751(1) 2012年5月  査読有り
    We present the discovery of a source with broadband infrared photometric characteristics similar to Sakurai's object. WISE J180956.27-330500.2 (hereafter J1810-3305) shows very red WISE colors, but a very blue 2MASS [K] versus WISE [W1 (3.4 mu m)] color. It was not visible during the IRAS era, but now has a 12 mu m flux well above the IRAS point-source catalog detection limit. There are also indications of variability in historical optical photographic plates as well as in multi-epoch AKARI mid-infrared measurements. The broadband infrared spectral energy distribution (SED) shape, post-IRAS brightening, and multiwavelength variability are all characteristics also shared by Sakurai's object-a post-asymptotic giant branch (post-AGB) star which underwent a late thermal pulse and recently ejected massive envelopes of dust that are currently expanding and cooling. Optical progenitor colors suggest that J1810-3305 may have been of late spectral class. Its dramatic infrared brightening and the detection of a late-type optical counterpart are consistent with a scenario in which we have caught an extremely massive dust ejection event (in 1998 or shortly before) during the thermal pulse of an AGB star, thus providing a unique opportunity to observe stellar evolution in this phase. J1810-3305 is the only source in the entire WISE preliminary data release with similar infrared SED and variability, emphasizing the rarity of such sources. Confirmation of its nature is of great importance.
  • H. Izumiura, T. Ueta, I. Yamamura, N. Matsunaga, Y. Ita, M. Matsuura, Y. Nakada, H. Fukushi, H. Mito, T. Tanabe, O. Hashimoto
    ASTRONOMY & ASTROPHYSICS 528 2011年4月  査読有り
    Context. Low-to intermediate-mass stars lose a significant fraction of their mass while they are on the asymptotic giant branch (AGB). This mass loss is considered to determine the final stages of their evolution. The material ejected from the stellar photosphere forms a circumstellar envelope in its surroundings. Layers of circumstellar envelope constitute the footprint of mass-loss history. Aims. Our aim is to probe the mass-loss history in the carbon star U Hya in the last similar to 10(4) years by investigating the distribution of dust in the circumstellar envelope with high spatial resolution. Methods. We observed U Hya in the far-infrared (FIR) at 65, 90, 140, and 160 mu m simultaneously, using the slow scan observing mode of the far-infrared surveyor (FIS) aboard the infrared astronomical satellite AKARI. It produced a map of similar to 10' x 40' in size in each band. Results. The FIS maps reveal remarkably circular, ring-like emission structure almost centered on the star, showing the presence of a detached, spherical dust shell. A hollow dust shell model gives the inner radius R-in of 101-107 '' [(2.5-2.6) x 1017 cm], thickness that covers a half of the total dust mass Delta R-hm of 16-23 '' [(3.8-5.6) x 10(16) cm], which gives Delta R-hm/R-in similar to 0.2, and the power-law index of the dust opacity distribution of 1.10-1.15. The dust mass in the shell is well-constrained to be (0.9-1.4) x 10(-4) (kappa(100)/25)(-1) M-circle dot, where kappa(100) is the dust absorptivity at 100 mu m in units of cm(2) g(-1). The dust mass-loss rate at R-in is found to be (1.89.6) x 10(-8)(kappa(100)/25)(-1)(v(e)/15) M-circle dot yr(-1), which shows that the total mass-loss rate in the shell is at least an order of magnitude higher than the current rate, where v(e) is the outflow velocity at R-in in units of km s(-1). An extension of FIR emission along PA similar to -70 degrees is found out to similar to 5' from the star, which is probably a ram-stripping wake by the ISM wind. We also find excess FIR emission that might indicate the earliest departure from spherical symmetry in the AGB mass loss inside the shell. Conclusions. The dust shell of U Hya is a hollow sphere and has an effective width that is narrower than the spatial resolution of the FIS. It could be formed as either a direct consequence of a thermal pulse, a result of two-wind interaction induced by a thermal pulse, a termination shock, or any combination of these processes.
  • Issei Yamamura, Takashi Tsuji, Toshihiko Tanabe, Tadashi Nakajima
    AKARI, A LIGHT TO ILLUMINATE THE MISTY UNIVERSE 418 143-+ 2009年  査読有り
    We report the results of the near-infrared spectroscopic observations of brown dwarfs with the AKARI/IRC. The spectra covering 2.5-5.0 mu m are significantly better quality than any previous observations ever made from the ground. So far spectra of seven objects are available. Their SEDs are consistent in principle with the prediction by the numerical model atmospheres including dust formation (Unified Cloudy Models; UCMs). We confirm the detection of CO absorption band in late-T dwarfs, supporting the idea of non-equilibrium processes contributing on the chemical abundance in these objects. In addition, we detect the CO2 band for the first time in brown dwarfs. The band commonly presents in the T-dwarfs. This could be a hint to understand the chemistry in the brown dwarf atmospheres.
  • Issei Yamamura, Masahiro Tanaka, Hidenori Takahashi, Sin'itirou Makiuti, Takanori Hirao, Takafumi Ootsubo, Mikako Matsuura, Kenich Okumura, Daisuke Ishihara, Takao Nakagawa, Hiroshi Murakami, Takashi Onaka, Hiroshi Shibai
    European Space Agency, (Special Publication) ESA SP (511) 35-38 2003年2月  
    The IRTS data archive has been in public since 2002. IRTS surveyed about 7 per cent of the whole sky with four instruments, which covered from 1.4 to 700 μm. Presently the archive includes the near- and mid-infrared low resolution spectral catalogues of point sources, and image maps in five wavelength bands in the far-infrared. The point source catalogues contains over 14 000 (near-infrared) and 500 (mid-infrared) sources. The majority of detected sources are late-type stars. These large samples of uniform spectra are especially useful for statistical studies of infrared properties of stars. The far infrared image maps are obtained for the 158 μm [C II] line, and continuum bands at 155, 250, 400, and 700 μm. Radiation from the diffuse interstellar components has been studied with these data. More data products will be available in a few year time-scale. The IRTS data can be accessed via ISAS's data archive service DARTS, URL: http://www.darts.isas.ac.jp/.
  • M Matsuura, Yamamura, I, AA Zijlstra, TR Bedding
    ASTRONOMY & ASTROPHYSICS 387(3) 1022-1031 2002年6月  査読有り
    We analyze ISO/SWS spectra of the RV Tau star R Scuti. The infrared spectra are dominated by H2O emission bands. The near- and mid-infrared excess is attributed to H2O; the dust contribution is less important. We also identify CO, SiO and CO2 bands. The various molecular emission bands originate from an extended atmosphere, an atmosphere above the photosphere. The extended atmosphere of R Sct is formed from matter which gradually have lifted up from the photosphere through the pulsations of the star. In contrast to the abundant molecules around the star, the silicate dust feature is weak and the dust mass-loss rate is only (M) over dot(d) = 10(-11) M-. yr(-1). This implies that there might be a process to inhibit dust formation from molecules. RV Tau stars are commonly considered as post-AGB stars. While a detached dust envelope around R Sct is consistent with such an interpretation, we show that its period evolution is slower than expected. We argue that R Sct may be a thermal-pulsing AGB star, observed in a helium-burning phase.
  • Yamamura, I, T de Jong
    ISO BEYOND THE PEAKS 456 155-160 2000年  査読有り
    The impact of the ISO/SWS on the study of AGE stars is reviewed. The ISO/SWS has provided high quality, intermediate resolution spectra covering a wide infrared wavelength range. These data enable us, for the first time, to perform an extensive study of the outer atmosphere and inner circumstellar regions of AGE stars. Many new and unexpected features hidden by the terrestrial atmosphere are detected, which raise new questions. We here particularly focus on the detection of dioxides in the O-rich stars, of C(3), C(2)H(2), and HCN in carbon stars, and of atomic / ionic fine-structure lines. We discuss the interpretation of these results and list problems to be solved.
  • Yamamura, I, T Onaka, T Tanabe, TL Roellig, LM Yuen
    PUBLICATIONS OF THE ASTRONOMICAL SOCIETY OF JAPAN 48(5) L65-L69 1996年10月  査読有り
    The mid-infrared spectrometer on board Infrared Telescope in Space has detected thousands of pointlike sources in the spectral range of 4.5-11.7 mu m. Extraction of point sources from the survey data has been carried out for the observing period after the spin-flip, where accurate pointing information is presently available, and 129 point sources have been extracted with signal-to-noise ratios greater than 3 throughout the MIRS spectral range. A two-color diagram of these objects, derived from bands of 5 mu m, 8 mu m, and 10 mu m of the sources, is presented. The sources can be classified into five groups on the diagram: visible late-type stars, stars with dust envelopes, stars with silicate emission, objects with the unidentified infrared (UIR) emission bands, and very peculiar red objects. With the help of the 5 mu m and 8 Irm colors, objects with the UIR bands can clearly be distinguished from objects without those features. The characteristics of the sources in each group are discussed based on the spectra.
  • YAMAMURA, I, T ONAKA, F KAMIJO, S DEGUCHI, N UKITA
    ASTROPHYSICAL JOURNAL 439(1) L13-L16 1995年1月  査読有り
    We report the results of mapping observations of a proto-planetary nebula CRL 2688 in the 13CO J = 1-0 line with a beam size of 4''.4 x 3''.9 with Nobeyama Millimeter Array. Emission of 13CO is extended by about 15'', which is about one-fourth of the CO envelope size obseved by single-dish telescopes. The channel velocity maps show that 13CO emission consists of three components: a spherically symmetric high-brightness core at the center, a less bright extended envelope with clumpy structure, and a high-velocity component near the center. The high-brightness central core is found to extend by about 10'' and to appear spherically symmetric. The disk- or torus-like structure which was previously observed by others in several molecular lines is not seen in the 13CO maps. This indicates that the gas density in the envelope does not vary much with the polar angle. The extended component is observed to spread along the symmetry axis. The peak positions of the red- and blueshifted features of the high-velocity component are found to be separated by about 3''.
  • YAMAMURA, I, KM SHIBATA, T KASUGA, S DEGUCHI
    ASTROPHYSICAL JOURNAL 427(1) 406-& 1994年5月  査読有り
    The circumstellar envelope of the carbon-rich star CRL 618 has been mapped by the (CO)-C-13 J = 1-0 transition with a resolution of about 5''.0 x 4''.3 with the Nobeyama Millimeter Array. Emission is extended in size by about 10'', and the distribution is approximately spherical. No strong elongation of (CO)-C-12 features along or perpendicular to the bipolar axis has been observed. Combining with the (CO)-C-12 J = 1-0 data that were taken before, we have created three-dimensional density and temperature profiles of the CRL 618 circumstellar envelope. For creating the three-dimensional model, it is assumed that the expansion velocity is constant and the large-velocity-gradient model is applicable. The former (CO)-C-12 observations show that the envelope of CRL 618 consists of complex features. On the basis of the present (CO)-C-13 observations, these features are interpreted as the temperature and density irregularities in the outer circumstellar shell. The comparison of the present results with the model density profile given by optical light-scattering maps is made.

MISC

 76
  • Yamamura, I, C Dominik, T de Jong, LBFM Waters, FJ Molster
    ASTRONOMY & ASTROPHYSICS 363(2) 629-639 2000年11月  
    The origin of silicate carbon stars has been a mystery ever since their discovery. We discuss here a full grating spectrum between 2.4 and 45 mum of the silicate carbon star V778 Cyg obtained by the ISO/SWS. The spectrum, taken about 14 years after the IRAS LRS observation, confirms the complex nature of the object. The spectrum is clearly divided into a short wavelength (lambda < 6.5 <mu>m), carbon-rich part and long-wavelength, oxygen-rich part. No obvious change of the 10 and 18 mum silicate features is observed between IRAS and ISO spectra, indicating that the silicate dust is in a steady structure. The 2.7 mum H2O band and the 15 mum CO2 bands are tentatively detected. The near-infrared part of the spectrum indicates that the present-day mass-loss rate is very low. The silicate features can only be fitted by optically thin dust emission from sub-micron size grains. The total oxygen-rich dust mass seen at infrared wavelengths is 2-10x10(-6) M., of which 3-50x10(-8) M. is warm (300-600 K). If the dust is heated by radiation from the central star, the dust should be located as close as about 12 stellar radii from the star. We suggest that the dust responsible for the emission features is in a steady outflow from the system. We show that the dust cannot be located in a circum-binary disk, but is stored in a disk around the companion star during the previous O-rich mass-loss phase. The duration of silicate emission is estimated as similar to 10(4) yr. It is compatible with the fact that not all J-type carbon stars show silicate emission. The evolution of the central star and formation of the disk in AGE binary systems largely depends on the orbital separation. V778 Cyg and other "IRAS discovered" silicate carbon stars probably have wide orbits. In such a case, a disk is formed around the companion. Close-binary systems such as the Red Rectangle form massive equatorial O-rich disks, and the evolution of the central star is largely influenced by the binarity.
  • J Cami, Yamamura, I, T de Jong, AGGM Tielens, K Justtanont, LBFM Waters
    ASTRONOMY & ASTROPHYSICS 360(2) 562-574 2000年8月  
    We present an analysis of the ISO/SWS full resolution scan between 12.5 and 16.5 mu m of the O-rich AGE star EP Aqr, exhibiting a number of strong CO(2) emission bands. We have developed a simple LTE model to calculate theoretical CO(2) spectra assuming a single-layer slab geometry and compared the SWS observations to this model in order to infer the physical properties of the extended atmosphere. The single layer slab model is able to reproduce the individual band profiles quite well with optically thick bands (column densities typically 10(18.5) cm(-2)). The derived excitation temperatures for the different bands are in the range T similar to 350 - 700 K in a region which extends from similar to 4 - 9R*. The fundamental CO(2) bending mode at 14.98 mu m furthermore shows evidence for an optically thin component arising from a much cooler (T similar to 100 K) and more extended (R(em) similar to 100R*) layer. The strong spectral signature of (13)CO(2) in the spectrum allows an (uncertain) determination of the (12)C/(13)C ratio similar to 10. The parameters derived for the CO(2) bands allow us to estimate the local temperature and density structure of the extended atmosphere. We find that the derived local gas temperatures are somewhat lower than predicted by hydrodynamical model calculations whereas the local gas densities are in good agreement with these models when using CO(2) abundances derived from chemical network calculations. The CO(2) layer extends from close to the stellar photosphere to the inner part of the dust forming region which makes it a unique new probe of the whole extended atmosphere and the region where dust formation takes place.
  • J Cami, Yamamura, I, T de Jong, AGGM Tielens, K Justtanont, LBFM Waters
    ASTRONOMY & ASTROPHYSICS 360(2) 562-574 2000年8月  
    We present an analysis of the ISO/SWS full resolution scan between 12.5 and 16.5 mu m of the O-rich AGE star EP Aqr, exhibiting a number of strong CO(2) emission bands. We have developed a simple LTE model to calculate theoretical CO(2) spectra assuming a single-layer slab geometry and compared the SWS observations to this model in order to infer the physical properties of the extended atmosphere. The single layer slab model is able to reproduce the individual band profiles quite well with optically thick bands (column densities typically 10(18.5) cm(-2)). The derived excitation temperatures for the different bands are in the range T similar to 350 - 700 K in a region which extends from similar to 4 - 9R*. The fundamental CO(2) bending mode at 14.98 mu m furthermore shows evidence for an optically thin component arising from a much cooler (T similar to 100 K) and more extended (R(em) similar to 100R*) layer. The strong spectral signature of (13)CO(2) in the spectrum allows an (uncertain) determination of the (12)C/(13)C ratio similar to 10. The parameters derived for the CO(2) bands allow us to estimate the local temperature and density structure of the extended atmosphere. We find that the derived local gas temperatures are somewhat lower than predicted by hydrodynamical model calculations whereas the local gas densities are in good agreement with these models when using CO(2) abundances derived from chemical network calculations. The CO(2) layer extends from close to the stellar photosphere to the inner part of the dust forming region which makes it a unique new probe of the whole extended atmosphere and the region where dust formation takes place.
  • The Astrophysical Journal 528(1) L33-L36 2000年1月  
  • Yamamura, I, K Kawaguchi, ST Ridgway
    ASTROPHYSICAL JOURNAL 528(1) L33-L36 2000年1月  
    We report the identification of SH Delta upsilon, 1 re-vibrational lines in the published high-resolution infrared spectrum of the S-type star R Andromeda. This is the first astronomical detection of this molecule. The lines show inverse P Cygni profiles, indicating infall motion of the molecular layer due to stellar pulsation. A simple spherical shell model with a constant infall velocity is adopted to determine the condition of the layer. It is found that a single excitation temperature of 2200 K reproduces the observed line intensities satisfactorily. SH is located in a layer from 1.0 to similar to 1.1 stellar radii, which is moving inward with a velocity of 9 km s(-1). These results are consistent with the previous measurements of CO Delta upsilon = 3 transitions. The estimated molecular abundance SH/H is 1 x 10(-7), consistent with a thermal equilibrium calculation.
  • J Cernicharo, Yamamura, I, E Gonzalez-Alfonso, T de Jong, A Heras, R Escribano, J Ortigoso
    ASTROPHYSICAL JOURNAL 526(1) L41-L44 1999年11月  
    We present the infrared Space Observatory/Short-Wavelength Spectrometer full grating resolution spectrum of IRC +10216, which is dominated by strong absorption/emission bands of C2H2 and HCN. All C2H2 bands and the strong near-infrared stretching bands of HCN are observed in absorption, whereas the fundamental, hot, and combination bands of HCN involving the nu(2) bending mode around 14 mu m are observed in emission. Particularly strong is the HCN nu(2) = 2(0) -> nu(2) = 1(1) vibrational transition at 14.3 mu m. The most plausible mechanism for such emission is the radiative pumping of molecules from the ground to the nu(2) = 2(0) state (7.1 mu m) followed by radiative decay: nu(2) = 2(0) -> v(2) = 1(1). We present detailed models for HCN that verify the efficiency of the mentioned effect. The HCN abundance inferred from these models is (1.5-3) x 10(-5).
  • J Cernicharo, Yamamura, I, E Gonzalez-Alfonso, T de Jong, A Heras, R Escribano, J Ortigoso
    ASTROPHYSICAL JOURNAL 526(1) L41-L44 1999年11月  
    We present the infrared Space Observatory/Short-Wavelength Spectrometer full grating resolution spectrum of IRC +10216, which is dominated by strong absorption/emission bands of C2H2 and HCN. All C2H2 bands and the strong near-infrared stretching bands of HCN are observed in absorption, whereas the fundamental, hot, and combination bands of HCN involving the nu(2) bending mode around 14 mu m are observed in emission. Particularly strong is the HCN nu(2) = 2(0) -> nu(2) = 1(1) vibrational transition at 14.3 mu m. The most plausible mechanism for such emission is the radiative pumping of molecules from the ground to the nu(2) = 2(0) state (7.1 mu m) followed by radiative decay: nu(2) = 2(0) -> v(2) = 1(1). We present detailed models for HCN that verify the efficiency of the mentioned effect. The HCN abundance inferred from these models is (1.5-3) x 10(-5).
  • FJ Molster, Yamamura, I, LBFM Waters, AGGM Tielens, T de Graauw, T de Jong, A de Koter, K Malfait, ME van den Ancker, H van Winckel, RHM Voors, C Waelkens
    NATURE 401(6753) 563-565 1999年10月  
    Silicate dust in the interstellar medium is observed to be amorphous(1), yet silicate dust in comets(2,3) and interplanetary dust particles(4) is sometimes partially crystalline. The dust in young stars(5,6) also appears to be partially crystalline. These clouds to a planetary system, it must undergo some processing, Here we report observations of highly crystalline silicate dust in the disks surrounding binary red-giant stars. The dust was created in amorphous form in the outer atmospheres of the red giants, and therefore must be processed in the disks to become crystalline. The temperatures in these disks are too low for the grains to anneal; therefore, some low-temperature process must be responsible. As the physical properties of the disks around young stars and red giants are similar, our results suggest that low-temperature crystallization of silicate grains also can occur in protoplanetary systems.
  • FJ Molster, Yamamura, I, LBFM Waters, AGGM Tielens, T de Graauw, T de Jong, A de Koter, K Malfait, ME van den Ancker, H van Winckel, RHM Voors, C Waelkens
    NATURE 401(6753) 563-565 1999年10月  
    Silicate dust in the interstellar medium is observed to be amorphous(1), yet silicate dust in comets(2,3) and interplanetary dust particles(4) is sometimes partially crystalline. The dust in young stars(5,6) also appears to be partially crystalline. These clouds to a planetary system, it must undergo some processing, Here we report observations of highly crystalline silicate dust in the disks surrounding binary red-giant stars. The dust was created in amorphous form in the outer atmospheres of the red giants, and therefore must be processed in the disks to become crystalline. The temperatures in these disks are too low for the grains to anneal; therefore, some low-temperature process must be responsible. As the physical properties of the disks around young stars and red giants are similar, our results suggest that low-temperature crystallization of silicate grains also can occur in protoplanetary systems.
  • M Matsuura, Yamamura, I, H Murakami, RM Freund, M Tanaka
    ASTRONOMY & ASTROPHYSICS 348(2) 579-583 1999年8月  
    The spectrometers onboard the Infrared Telescope in Space (IRTS) reveal water vapor absorption in early M-type stars, as early as M2. Previous observations detected H2O vapor absorption only in stars later than M6, with the exception of the recent detection of H2O in beta Peg (M2.5 II-III). In our sample of 108 stars, 67 stars have spectral types earlier than M6. The spectral types are established by means of their near-infrared colors on a statistical basis. Among the 67 stars of spectral types earlier than M6, we find water vapor absorption in six stars. The observed absorption features are interpreted using a local thermodynamic equilibrium model. The features are reasonably fitted by model spectra with excitation temperatures of 1000-1500 K and water column densities of 5 x 10(19) to 1 x 10(20) cm(-2). These numbers, imply that the H2O molecules are present in a region of the atmosphere, located above the photosphere. Furthermore, our analysis shows a good correlation between the H2O absorption band strength, and the mid-infrared excess due to the circumstellar dust. We discuss the relation between the outer atmosphere and the mass loss.
  • Yamamura, I, T de Jong, J Cami
    ASTRONOMY & ASTROPHYSICS 348(3) L55-L58 1999年8月  
    The ISD/SWS spectrum of o Cet taken at its maximum exhibits an absorption-like feature between 3.5 and 4.0 mu m We present evidence that the feature is due to emission of H2O and SiO molecules, in a layer extended to about two stellar radii with an excitation temperature of 2000 K. These hot molecules are also observed in a spectrum of Z Cas near minimum, but this time in absorption. A simple plane-parallel model is used to fit the spectra of these two stars. The H2O column densities and excitation temperatures in the layers are found to be similar in both stars. The difference of the H2O band is thus primarily due to the layer size. The H2O layers seem to be more extended at visual maximum, probably related to the stellar pulsation. The estimated lower limit to the local gas density in the layers of similar to 10(11) cm(-3) is in good agreement with theoretical predictions from dynamical model atmospheres.
  • M Matsuura, Yamamura, I, H Murakami, RM Freund, M Tanaka
    ASTRONOMY & ASTROPHYSICS 348(2) 579-583 1999年8月  
    The spectrometers onboard the Infrared Telescope in Space (IRTS) reveal water vapor absorption in early M-type stars, as early as M2. Previous observations detected H2O vapor absorption only in stars later than M6, with the exception of the recent detection of H2O in beta Peg (M2.5 II-III). In our sample of 108 stars, 67 stars have spectral types earlier than M6. The spectral types are established by means of their near-infrared colors on a statistical basis. Among the 67 stars of spectral types earlier than M6, we find water vapor absorption in six stars. The observed absorption features are interpreted using a local thermodynamic equilibrium model. The features are reasonably fitted by model spectra with excitation temperatures of 1000-1500 K and water column densities of 5 x 10(19) to 1 x 10(20) cm(-2). These numbers, imply that the H2O molecules are present in a region of the atmosphere, located above the photosphere. Furthermore, our analysis shows a good correlation between the H2O absorption band strength, and the mid-infrared excess due to the circumstellar dust. We discuss the relation between the outer atmosphere and the mass loss.
  • Yamamura, I, T de Jong, J Cami
    ASTRONOMY & ASTROPHYSICS 348(3) L55-L58 1999年8月  
    The ISD/SWS spectrum of o Cet taken at its maximum exhibits an absorption-like feature between 3.5 and 4.0 mu m We present evidence that the feature is due to emission of H2O and SiO molecules, in a layer extended to about two stellar radii with an excitation temperature of 2000 K. These hot molecules are also observed in a spectrum of Z Cas near minimum, but this time in absorption. A simple plane-parallel model is used to fit the spectra of these two stars. The H2O column densities and excitation temperatures in the layers are found to be similar in both stars. The difference of the H2O band is thus primarily due to the layer size. The H2O layers seem to be more extended at visual maximum, probably related to the stellar pulsation. The estimated lower limit to the local gas density in the layers of similar to 10(11) cm(-3) is in good agreement with theoretical predictions from dynamical model atmospheres.
  • Deguchi Shuji, Fujii Takahiro, Izumimura Hideyuki, MATSUMOTO Shigeru, NAKADA Yoshikazu, WOOD Peter R., YAMAMURA Issei
    PASJ : publications of the Astronomical Society of Japan 51(3) 355-361 1999年  
  • Yamamura, I, T de Jong, T Onaka, J Cami, LBFM Waters
    ASTRONOMY & ASTROPHYSICS 341(1) L9-L12 1999年1月  
    We report the discovery of the upsilon(3) band of SO2 at 7.3 mu m in the ISO/SWS spectra of oxygen-rich AGB stars. The band is clearly detected in three stars, UX Cyg, o Cet and T Cep, and marginally detected in at least four other stars. The band is seen in absorption in UX Cyg, while it is in emission in o Get. Seven spectra of T Cep taken at different phases show that the feature changes from emission to absorption on a time scale of twice the pulsation period. Using an LTE model, we find that the excitation temperature of SO2 is typically 600 K, and that in T Cep the molecule occupies a region with dimensions of several stellar radii. The total number of molecules contained in this region is of order 10(47), which requires a local gas density of at least 10(9) H-2 cm(-3), and possibly up to 10(11) H-2 cm(-3) depending on the SO2 abundance. The variation with phase of the T Cep spectra can be explained by photodissociation of SO2 molecules by soft UV photons.
  • Yamamura, I, T de Jong, T Onaka, J Cami, LBFM Waters
    ASTRONOMY & ASTROPHYSICS 341(1) L9-L12 1999年1月  
    We report the discovery of the upsilon(3) band of SO2 at 7.3 mu m in the ISO/SWS spectra of oxygen-rich AGB stars. The band is clearly detected in three stars, UX Cyg, o Cet and T Cep, and marginally detected in at least four other stars. The band is seen in absorption in UX Cyg, while it is in emission in o Get. Seven spectra of T Cep taken at different phases show that the feature changes from emission to absorption on a time scale of twice the pulsation period. Using an LTE model, we find that the excitation temperature of SO2 is typically 600 K, and that in T Cep the molecule occupies a region with dimensions of several stellar radii. The total number of molecules contained in this region is of order 10(47), which requires a local gas density of at least 10(9) H-2 cm(-3), and possibly up to 10(11) H-2 cm(-3) depending on the SO2 abundance. The variation with phase of the T Cep spectra can be explained by photodissociation of SO2 molecules by soft UV photons.
  • Ootsubo T., Onaka T., Yamamura I., TANABE T., ROELLIG T. L., CHAN K. -W., MATSUMOTO T.
    Earth, planets and space 50(6) 507-511 1998年7月  
  • K Justtanont, H Feuchtgruber, T de Jong, J Cami, LBFM Waters, Yamamura, I, T Onaka
    ASTRONOMY & ASTROPHYSICS 330(1) L17-L20 1998年2月  
    We have detected strong emission lines at 13.48, 13.87, 14.97, 15.40 and 16.28 mu m in the ISO/SWS spectra of O-rich AGE stars. These lines are only found in the spectra of Miras and semi-regular variables when they also show the 13 mu m dust emission feature. The lines appear just resolved in the high-resolution (AOT06, resolution similar to 1500) SWS spectra that we recently obtained. Here we report the identification of these emission lines as the Q-branches of re-vibrational transitions in CO2 molecules. This identification is corroborated by our SWS Fabry-Perot observation of the 13.87 mu m line in W Hya where individual Q-branch components of the 10(0)0 Sigma(g)(+) - 01(1)0 Pi(u) transition of CO2 have been detected. The 15.40 mu m line is probably due to (CO2)-C-13. We speculate that the simultaneous occurence of the 13 mu m dust feature and the CO2 emission lines indicates the existence of a warm (similar to 650-1250 K) gas layer close to the star where both the 13 mu m dust and the CO2 emission lines are formed.
  • 大坪貴文, 尾中敬, 山村一誠, 田辺俊彦, ROELLIG T L, CHAN K-W, 松本敏雄
    日本天文学会年会講演予稿集 1998 1998年  
  • 山村 一誠
    天文月報 90(6) 259-265 1997年5月20日  
  • Yamamura, I, T Onaka, F Kamijo, S Deguchi, N Ukita
    ASTROPHYSICAL JOURNAL 465(2) 926-939 1996年7月  
    We have studied the proto-planetary nebula CRL 2688 by mapping observations of the (CO)-C-13 J = 1-0 line. Data obtained by single-dish (Nobeyama 45 m) and interferometric (Nobeyama Millimeter Array) observations are combined and reduced to maps of the whole flux of (CO)-C-13 emission in the envelope. The resultant maps reveal that weak (CO)-C-13 emission is extended by about 20 '' (corresponding to 3 x 10(17) cm) from the central star. Part of the extended emission spreads toward the south of the source, although no counterpart is seen in the north. The mass of this component is estimated to be about 0.08 M.. Numerical model analyses of the velocity-channel maps are performed to obtain a three-dimensional density distribution in the envelope. They indicate that the mass loss of the central star was drastically increased about 3000 yr ago, reached a maximum rate of about 3 x 10(-4) M. yr(-1), and then abruptly stopped approximately 200 yr ago. The present (CO)-C-13 observations show no evidence for the presence of a large axisymmetric disk in the bright core region. The disk, which is inferred from the shape of the bipolar reflection nebula at the optical and near-infrared wavelengths, may be very small, less than a few arcseconds in size. It is suggested that the high-velocity flow detected in the (CO)-C-13 interferometric observations originates from the gas in the thick envelope heated by the shock with collimated outflows.
  • Yamamura, I, T Onaka, F Kamijo, S Deguchi, N Ukita
    ASTROPHYSICAL JOURNAL 465(2) 926-939 1996年7月  
    We have studied the proto-planetary nebula CRL 2688 by mapping observations of the (CO)-C-13 J = 1-0 line. Data obtained by single-dish (Nobeyama 45 m) and interferometric (Nobeyama Millimeter Array) observations are combined and reduced to maps of the whole flux of (CO)-C-13 emission in the envelope. The resultant maps reveal that weak (CO)-C-13 emission is extended by about 20 '' (corresponding to 3 x 10(17) cm) from the central star. Part of the extended emission spreads toward the south of the source, although no counterpart is seen in the north. The mass of this component is estimated to be about 0.08 M.. Numerical model analyses of the velocity-channel maps are performed to obtain a three-dimensional density distribution in the envelope. They indicate that the mass loss of the central star was drastically increased about 3000 yr ago, reached a maximum rate of about 3 x 10(-4) M. yr(-1), and then abruptly stopped approximately 200 yr ago. The present (CO)-C-13 observations show no evidence for the presence of a large axisymmetric disk in the bright core region. The disk, which is inferred from the shape of the bipolar reflection nebula at the optical and near-infrared wavelengths, may be very small, less than a few arcseconds in size. It is suggested that the high-velocity flow detected in the (CO)-C-13 interferometric observations originates from the gas in the thick envelope heated by the shock with collimated outflows.
  • H IZUMIURA, R CATCHPOLE, S DEGUCHI, O HASHIMOTO, Y NAKADA, T ONAKA, T ONO, K SEKIGUCHI, N UKITA, YAMAMURA, I
    ASTROPHYSICAL JOURNAL SUPPLEMENT SERIES 98(1) 271-294 1995年5月  
    We have surveyed Galactic bulge IRAS sources in the strips between -15 degrees < l < 15 degrees and 4 degrees < \b\ < 5 degrees in the SiO J = 1-0 upsilon = 1 and 2 transitions. The sources were selected from the IRAS Point Source Catalog based on the IRAS 25/12 mu m flux density ratio, extracting dust-enshrouded objects at a distance of about 8 kpc. The SiO masers were detected in 62 of 93 sources surveyed in these strips. The JHKL photometric data (1.2, 1.6, 2.2, and 3.4 mu m) were also obtained for 85 sources. Because distances to the IRAS sources in these strips are not known, we have evaluated the distance based on the observed luminosity. The probability of the objects being a bulge source is calculated assuming that the luminosity function of these infrared sources is the same as that of previously observed \b\ = 7 degrees-8 degrees sources. The contamination due to foreground sources in the sample is minimized by excluding sources with the bulge probability less than 50%. The SiO maser properties of the \b\ = 4 degrees-5 degrees sources are found to be very similar to those of \b\ = 7 degrees-8 degrees sources. No systematic difference between bulge and disk sources is found for the SiO J = 1-0 upsilon = 2/1 intensity ratio. The average rotation rate of the bulge stellar system for the \b\ = 4 degrees-5 degrees sources is found to be 10.8 (+/-2.6) km s(-1) deg(-1), indicating no sign of increase of the rotation rate at this strip compared with the rate obtained for the \b\ = 7 degrees-8 degrees sources. On the contrary, the velocity dispersions of stars, 91.0 +/- 9.5 km s(-1), for the \b\ = 4 degrees-5 degrees sources seems appreciably larger than the dispersion, 72.5 +/- 8.9 km s(-1) obtained for the \b\ = 7 degrees-8 degrees sources. A small, systematic velocity shift of the radial velocities is found between the south and north strip sources. If this shift is interpreted as due to a tilt of the bulge, the tilt angle of the bulge rotation axis to the Galactic circle would be 8(-31)(+27) deg, which is slightly smaller than the value obtained for the \b\ = 7 degrees-8 degrees sources.
  • H. Izumiura, S. Deguchi, O. Hashimoto, Y. Nakada, T. Onaka, T. Uno, N. Ukita, I. Yamamura
    Astrophysical Journal 437(1) 419-435 1994年12月10日  
    We have surveyed Galactic bulge IRAS sources in the strips between -15° &lt l &lt 15° and 7° &lt |b| &lt 8° in the SiO J = 1-0 ν = 1 and 2 transitions. The sources were selected from the IRAS Point Source Catalogue based on the IRAS 12 and 25 μm flux densities, extracting dust-enshrouded objects at a distance of 8 kpc. SiO masers were detected in 53 of the 91 sources surveyed in these strips. Because distances to the IRAS sources in these strips have been known from the period-luminosity relation and periods of intensity variation at infrared wavelengths measured by others, the contamination by foreground sources in the sample can be checked relatively easily and the uncertainty in deriving physical parameters of the bulge is minimized. The detection rate of SiO masers does not depend much on the infrared colors in the selected color range (logarithm of the IRAS 25 to 12 μm flux density ratio between -0.15 and 0.3) and the detection rate increases with the 12 μm flux density of the IRAS sources. It has been found that the intrinsic SiO maser intensity depends weakly on the mass-loss rate for the bulge and disk SiO maser sources. No systematic difference of the SiO maser properties is found between bulge and disk sources. The radial velocities in the northern strip are shifted systematically from those in the southern strip by about 50 km s-1. If this velocity shift is interpreted as due to a tilt of the bulge rotation axis to the galactic longitude circle, the tilt angle of the rotation of the bulge would be 18°(-14°+18°). The angular rotation velocity of the bulge stellar system is 7.3 × 108 rad yr-1 (implying the rotation period of 8.6 × 107 yr). A Galactic top view of the distribution and the velocity vectors of the bulge SiO masers is given.
  • YAMAMURA, I, T ONAKA, F KAMIJO, H IZUMIURA, S DEGUCHI
    PUBLICATIONS OF THE ASTRONOMICAL SOCIETY OF JAPAN 45(4) 573-585 1993年  
    We have observed the carbon star S Sct in the CO J = 1-0 line with the 16'' beam of the 45-m radio telescope at Nobeyama Radio Observatory. The spectrum towards the star exhibits a sharp double spike, and the spectra at the offset positions (20'', 40'', and 60'') show that the intensities and the velocity widths vary with the offset, indicating that the circumstellar envelope of S Sct is detached. Model calculations of the CO line intensities taking into account the non-LTE (Local Thermodynamical Equilibrium) effects lead us to conclude that the inner radius of the circumstellar shell of the star is 5.2 x 10(17) cm, that the thickness of the circumstellar shell is less-than-or-equal-to 0.20 x 10(17) cm (which is by about a factor of 3 thinner than previously thought), and that the shell was formed by an extremely high-mass-loss event (a mass-loss rate of greater-than-or-equal-to 1.3 x 10(-4) M. yr-1) about 10(4) yr ago. The unusually high rate of mass loss could explain the fact that only three carbon stars with detached shells have ever been detected by CO observations. A new hypothesis concerning carbon star formation by Willems and de Jong (1988, AAA 065.070) suggests that optically bright carbon stars are objects in the intermediate phase between the termination of the oxygen-rich mass-loss phase and the beginning of the mass loss of the infrared carbon star phase. The derived time scale after the mass-loss termination of S Sct (10(4) yr) is similar to the estimated lifetime of optically bright carbon stars in their scenario.
  • YAMAMURA, I, T ONAKA, F KAMIJO, H IZUMIURA, S DEGUCHI
    PUBLICATIONS OF THE ASTRONOMICAL SOCIETY OF JAPAN 45(4) 573-585 1993年  
    We have observed the carbon star S Sct in the CO J = 1-0 line with the 16'' beam of the 45-m radio telescope at Nobeyama Radio Observatory. The spectrum towards the star exhibits a sharp double spike, and the spectra at the offset positions (20'', 40'', and 60'') show that the intensities and the velocity widths vary with the offset, indicating that the circumstellar envelope of S Sct is detached. Model calculations of the CO line intensities taking into account the non-LTE (Local Thermodynamical Equilibrium) effects lead us to conclude that the inner radius of the circumstellar shell of the star is 5.2 x 10(17) cm, that the thickness of the circumstellar shell is less-than-or-equal-to 0.20 x 10(17) cm (which is by about a factor of 3 thinner than previously thought), and that the shell was formed by an extremely high-mass-loss event (a mass-loss rate of greater-than-or-equal-to 1.3 x 10(-4) M. yr-1) about 10(4) yr ago. The unusually high rate of mass loss could explain the fact that only three carbon stars with detached shells have ever been detected by CO observations. A new hypothesis concerning carbon star formation by Willems and de Jong (1988, AAA 065.070) suggests that optically bright carbon stars are objects in the intermediate phase between the termination of the oxygen-rich mass-loss phase and the beginning of the mass loss of the infrared carbon star phase. The derived time scale after the mass-loss termination of S Sct (10(4) yr) is similar to the estimated lifetime of optically bright carbon stars in their scenario.

書籍等出版物

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講演・口頭発表等

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共同研究・競争的資金等の研究課題

 16