arXiv subjects

Masayuki Umemura

Publications and source records attributed to Masayuki Umemura.

At least 73 records · Page 4Linked to original sources

arXiv2004

The Nature of Lya Blobs: Supernova-Dominated Primordial Galaxies

We consider a forming galaxy undergoing multitudinous supernova (SN) explosions, as a possible model of \lya blobs (LABs). For this purpose, an ultra--high resolution hydrodynamic simulation is performed using $1024^3$ grid points, where SN remnants are resolved with sufficient accuracy. It is found that multiple SN explosions produce kpc--size expanding hot bubbles, which drive cool, dense shells by strong shock. The colliding high--density cooling shells radiate intensive \lya emission, resulting in a high \lya luminosity of $\sim10^{43}$ erg s$^{-1}$, comparable to the observed level in LABs. Also, recently discovered bubbly features in some LABs are quite similar to the structure predicted in the present simulation. Furthermore, the result demonstrates that LABs are representative of evolving primordial galaxies; they could hold direct information on the early chemical enrichment of galaxies, contrary to present--day galaxies which have undergone intense recycling of interstellar matter, thus erasing most of the early chemical history. It turns out that the metal mixing proceeds in a very inhomogeneous fashion, so that there appears a large spread of metallicity, that is,$[{\rm Fe/H}] \approx 0 {\rm ~to} -5$ or $[{\rm O/H}] \approx 1 {\rm ~to} -4$. Hence, the early galactic chemical evolution may have proceeded in a different manner from that hitherto considered in one--zone models.

astro-ph↗

arXiv2004

Gas stripping by radiation drag from an interstellar cloud

We perform two-dimensional hydrodynamic simulation on the gas stripping by radiation drag from an interstellar cloud moving in uniform radiation fields. To properly include relativistic radiation drag, the radiation hydrodynamic equation is solved with taking into account the dilution of radiation fields by optical depth of the cloud. As a result, it is found that the optically-thin surface layers are effectively stripped by radiation drag from an optically-thick gas cloud, and simultaneously stripped gas loses momentum. The momentum loss time-scale is found to be on the order of $10^{8}$ years under intensive radiation fields which are expected in the early phase of galaxy evolution. The present results show that the radiation drag is an effective mechanism to extract angular momentum from interstellar medium and allows it to accrete onto the galactic center. The mass accretion driven by radiation drag may lead to the formation of a central supermassive black hole.

astro-ph↗

arXiv2004

Effects of Early Cosmic Reionization on the Substructure Problem in Galactic Halo

Recent observations on the cosmic microwave background by Wilkinson Microwave Anisotropy Probe(WMAP) strongly suggest that the reionization of the universe took place quite early (z \sim 17). On the other hand, it has been pointed out that the cold dark matter cosmology suffers from the substructure problem that subgalactic halos are overproduced than the observed dwarf galaxies in the Local Group. In this paper, as a potential mechanism to solve this problem, we consider the feedback effects of the early reionization on the formation of small-scale structures. For this purpose, we perform 3D radiation hydrodynamic simulations with incorporating the radiative transfer for ionizing photons. As a result, it is found that the early reionization is so devastating for low-mass systems with M_{vir}\la 10^8 M_\odot or v_{circ}\la 20km/s, and almost all gas is photo-evaporated in more than 95% of low-mass systems. Such a strong negative feedback on the formation of low-mass galaxies may solve the substructure problem and support the picture that Local Group dwarf galaxies are descendants of the more massive halos that experienced and survived tidal stripping.

astro-ph↗

arXiv2003

Why Massive Black Holes are Small in Disk Galxies?

A potential mechanism is proposed to account for the fact that supermassive black holes (SMBHs) in disk galaxies appear to be smaller than those in elliptical galaxies in the same luminosity range. We consider the formation of SMBHs by radiation drag (Poynting-Robertson effect), which extracts angular momentum from interstellar matter and thereby drives the mass accretion onto a galactic center. In particular, we quantitatively scrutinize the efficiency of radiation drag in a galaxy composed of bulge and disk, and elucidate the relation between the final mass of SMBH and the bulge-to-disk ratio of the galaxy. As a result, it is found that the BH-to-galaxy mass ratio, $M_{\rm BH}/M_{\rm galaxy}$, decreases with a smaller bulge-to-disk ratio, due to the effects of geometrical dilution and opacity, and is reduced maximally by two orders of magnitude, resulting in $M_{\rm BH}/M_{\rm galaxy}\approx 10^{-5}$. In contrast, if only the bulge components in galaxies are focused, the BH-to-bulge mass ratio becomes $M_{\rm BH}/M_{\rm bulge}\approx 10^{-3}$, which is similar to that found in elliptical galaxies. Thus, it turns out that the mass of SMBH primarily correlates with a bulge, not with a disk, consistently with observational data.

astro-ph↗

arXiv2003

Quasar Mesolensing - Direct Probe to Substructures around Galaxies -

Recently, ``CDM crisis'' is under discussion. The main point of this crisis is that number of substructures presented by cosmological N-body simulations based on CDM scenario for structure formation is much larger than observed substructures. Therefore, it is crucial for this crisis to discriminate whether expected number of CDM substructures really exist but non-luminous or do not exist. In this paper, we present a new idea to detect such invisible substructures by utilizing a gravitational lensing. Here, we consider quasars that are gravitationally lensed by a foreground galaxy. A substructure around the lensing galaxy may superposed on one of the lensed images of such quasars. In this situation, additional image splitting should occur in the image behind the substructure, and further multiple images are created. This is ``quasar mesolensing''. We estimate separation and time delay between further multiple images due to quasar mesolensing. The expected value is $1 \sim 30$ milli-arcsecond for the separation and future fine resolution imaging enable us to find invisible substructures, and is $1 \sim 10^3$ second for the time delay and high-speed monitoring of such quasar will be able to find ``echo''-like variation due to quasar mesolensing in intrinsic variability of the quasar. Furthermore, we evaluate that the optical depth for the quasar mesolensing is $\sim 0.1$. Consequently, if we monitor a few multiple quasars, we can find ``echo''-like variation in one of the images after intrinsic flux variations of quasars.

astro-ph↗

arXiv2003

Formation of Dwarf Galaxies during the Cosmic Reionization

We reanalyze the photoevaporation problem of subgalactic objects irradiated by UVB radiation in a reionized universe. For the purpose, we perform three-dimensional radiation smoothed-particle-hydrodynamics calculations, where the radiative transfer is solved by a direct method and also the non-equilibrium chemistry of primordial gas including H$_2$ molecules is incorporated. Attention is concentrated on radiative transfer effects against UVB for the formation of subgalactic objects with $T_{\rm vir}\la 10^4$K. We consider the reionization model with $z_{\rm reion} \approx 7$ and also the earlier reionization model ($z_{\rm reion} \approx 17$) inferred by the WMAP. We find that the star formation is suppressed appreciably by UVB, but baryons at high-density peaks are self-shielded even during the reionization, forming some amount of stars eventually. In that sense, the photoevaporation for subgalactic systems is not so perfect as argued by one-dimensional spherical calculations. The final stellar fraction depends on the collapse epoch and the mass of system, but almost regardless of the reionization epoch. For instance, a few tenths of formed stars are born after the cosmic reionization in $z_{\rm reion} \approx 7$ model, while more than 90% stars are born after the reionization in the WMAP reionization model. Thus, effects of UVB feedback on the substructure problem with CDM scenario should be evaluated with careful treatment of the radiative transfer. The star clusters formed at high-density peaks coalesce with each other in a dissipationless fashion in a dark matter potential, resultantly forming a spheroidal system. As a result, these low-mass galaxies have large mass-to-light ratios such as observed in dwarf spheroidals in the Local Group.

astro-ph↗

arXiv2003

The Growth of Supermassive Black Holes and QSO Formation

A novel mechanism to build up a supermassive black hole (SMBH) is proposed. Here, relativistic radiation-hydrodynamic processes are considered from a galactic scale to a horizon scale. In the present scenario, the mass of a SMBH is predicted to be in proportion to the bulge mass, and it turns out that the SMBH-to-bulge mass ratio is basically determined by the nuclear energy conversion efficiency from hydrogen to helium, $ε=0.007$. The BH hierarchy is also addressed in relation to the BH formation in globular clusters. Futhermore, a new picture for QSO formation is proposed based on the present SMBH formation scenario. It is predicted that a host luminosity-dominant ``proto-QSO phase'' exists before the QSO phase, and the proto-QSO phase is preceded by an optically-thick ultraluminous infrared galaxy (ULIRG) phase.

astro-ph↗

arXiv2002

A Search for Lyman alpha Emitters at Redshift 3.7

We present the results of a survey for emission-line objects based on optical intermediate-band ($λ_{\rm c}$ = 5736 Å~ and $Δλ$ = 280 Å) and broad-band ($B$, $V$, $R$, and $i^\prime$) observations of the Subaru/XMM-Newton Deep Field on the 8.2 m Subaru telescope with the Subaru Prime Focus Camera, Suprime-Cam. All the data were obtained during the guaranteed time observations of the Suprime-Cam instrument. The intermediate-band image covered a sky area with 10\minpoint62 $\times 12\minpoint40 \approx 132$ arcmin$^2$ in the Subaru/XMM-Newton Deep Field (Ouchi et al.). Using this image, we have found 23 emission-line sources whose observed emission-line equivalent widths are greater than 250 Å. Their optical multicolor properties indicate that six emission-line sources are Ly$α$ emitters at $z \approx$ 3.7 ($Δz \approx 0.22$). They are either intense starburst galaxies or active galactic nuclei like quasars at $z \approx$ 3.7. Two more emission-line sources may also be Ly$α$ emitters at $z \approx$ 3.7 although their multicolor properties are marginal. Among the remaining 15 emission-line objects, eight objects appear strong emission-line galaxies at lower redshift; e.g., [O {\sc ii}] $λ$3727 emitters at $z \approx 0.54$, H$β$ at $z \approx 0.18$, or [O {\sc iii}]$λ$5007 emitters at $z \approx 0.15$. The remaining seven objects are unclassified because they are too faint to be detected in broad-band images. We discuss observational properties of these strong emission-line sources. In particular, our data allow us to estimate the star formation density at $z \approx 3.7$ for the first time.

astro-ph↗

arXiv2002

Proto-Quasars:Physical States and Observable Properties

Based on the radiation hydrodynamical model for the black hole(BH) growth,incorporated with the chemical evolution of the early-type host galaxy, we construct the coevolution model of a QSO BH and the host galaxy. As a result, it is found that after a galactic wind epoch,the luminosity is shifted from the host-dominant phase to the AGN-dominant phase (QSO phase) in the timescale of a few $10^{8}$ years.The former phase corresponds to the early stage of growing BH, and can be regarded as a ``proto-QSO'' phase. It has observable characteristic properties (detail inthis paper).By comparing these predictions with recent observations, radio galaxies are a possible candidate for proto-QSOs.Also, it is anticipated that the proto-QSO phase is preceded by an optically thick phase, which may correspond to ULIRGs.In this phase, $M_{\rm BH}/M_{\rm bulge}$ is predicted to be much less than $10^{-3}$ and grow with metallicity.Moreover, as precursors of ULIRGs, optically-thin star-forming galaxies are predicted. These may be in the assembly phase of Lyman break galaxies (LBGs) or Ly$α$ emitters.

astro-ph↗

arXiv2002

Does the Slim-Disk Model Correctly Consider Photon-Trapping Effects?

We investigate the photon-trapping effects in the super-critical black hole accretion flows by solving radiation transfer as well as the energy equations of radiation and gas. It is found that the slim-disk model generally overestimates the luminosity of the disk at around the Eddington luminosity (L_E) and is not accurate in describing the effective temperature profile, since it neglects time delay between energy generation at deeper inside the disk and energy release at the surface. Especially, the photon-trapping effects are appreciable even below L ~ L_E, while they appear above ~ 3L_E according to the slim disk. Through the photon-trapping effects, the luminosity is reduced and the effective temperature profile becomes flatter than r^{-3/4} as in the standard disk. In the case that the viscous heating is effective only around the equatorial plane, the luminosity is kept around the Eddington luminosity even at very large mass accretion rate, Mdot>>L_E/c^2. The effective temperature profile is almost flat, and the maximum temperature decreases in accordance with rise in the mass accretion rate. Thus, the most luminous radius shifts to the outer region when Mdot/(L_E/c^2) >> 10^2. In the case that the energy is dissipated equally at any heights, the resultant luminosity is somewhat larger than in the former case, but the energy-conversion efficiency still decreases with increase of the mass accretion rate, as well. The most luminous radius stays around the inner edge of the disk in the latter case. Hence, the effective temperature profile is sensitive to the vertical distribution of energy production rates, so is the spectral shape. Future observations of high L/L_E objects will be able to test our model.

astro-ph↗

arXiv2002

The Stellar Initial Mass Function in Primordial Galaxies

In the context of star formation through fragmentation of an extremely metal-deficient protogalactic cloud, the gravitational collapse of filamentary gas clouds is explored with 1D numerical hydrodynamics coupled with non-equilibrium chemistry of H$_2$ and HD. It is found that the cloud evolution is governed mainly by the initial central density ($n_{\rm c,0}$) and H$_2$ abundance ($x_{\rm H_2,0}$). In particular, the evolution of low-density filaments bifurcates at a threshold H$_2$ abundance of $x_{\rm H_2,cr}\simeq 3 \times 10^{-3}$, beyond which HD cooling overwhelms H$_2$ cooling. The contraction of a low density filament with $x_{\rm H_2, 0}\gtrsim x_{\rm H_2,cr}$ is strongly decelerated when $n_{\rm c}$ reaches a critical density of HD, and the filament is expected to fragment at $\sim 10^{7}$ cm$^{-3}$. The fragment mass is lowered to be $\approx 10M_\odot$. In contrast, the contraction of a low density filament with $x_{\rm H_2, 0}\lesssim x_{\rm H_2,cr}$ is regulated by H$_2$ cooling. In this case, the fragment mass is as high as $\approx 10^2M_\odot$. For a high-density filament, the cloud evolution is governed by H$_2$ cooling. The fragmentation is not expected to take place until the cloud becomes opaque in H$_2$ lines at $n_{\rm c,0}\sim 10^{12-13}$ cm$^{-3}$, so that the fragment mass is reduced to 1-2 M$_\odot$. As a result, the stellar IMF could be bimodal and deficient in sub-solar mass stars, where the high mass peak is around $10M_\odot$ or $10^2M_\odot$, dependently on $n_{\rm c,0}$ and $x_{\rm H_2,0}$.

astro-ph↗

arXiv2001

Radiation drag driven mass accretion in clumpy interstellar medium: implications for the supermassive black hole-to-bulge relation

We quantitatively scrutinize the effects of the radiation drag arising from the radiation fields in a galactic bulge in order to examine the possibility that the radiation drag could be an effective mechanism to extract angular momentum in a spheroidal system like a bulge and allow plenty of gas to accrete onto the galactic center. For this purpose, we numerically solve the relativistic radiation hydrodynamical equation coupled with the accurate radiative transfer and quantitatively assess the radiation drag efficiency. As a result, we find that in an optically thick regime the radiation drag efficiency is sensitively dependent on the density distributions of interstellar medium (ISM). The efficiency drops according to $τ_{\rm T}^{-2}$ in an optically thick {\it uniform} ISM, where $τ_{\rm T}$ is the total optical depth of the dusty ISM, whereas the efficiency remains almost constant at a high level if the ISM is {\it clumpy}. Hence, if the bulge formation begins with a star formation event in a clumpy ISM, the radiation drag will effectively work to remove the angular momentum and the accreted gas may form a supermassive black hole. As a natural consequence, this mechanism reproduces a putative linear relation between the mass of a supermassive black hole and the mass of a galactic bulge, although further detailed modeling for stellar evolution is required for the more precise prediction.

astro-ph↗

arXiv2001

A Radiation-Hydrodynamical Model for Supermassive Black Hole-to-Bulge Mass Relation and Quasar Formation

As a potential mechanism to build up supermassive black holes (BHs) in a spheroidal system, we consider the radiation drag effect by bulge stars, which extracts angular momentum from interstellar gas and thus allows the gas to accrete onto the galactic center. With incorporating radiation hydrodynamical equation with simple stellar evolution, it is shown that the BH-to-bulge mass ratio, $f_{BH}$, is basically determined by a fundamental constant, that is, the energy conversion efficiency for nuclear fusion of hydrogen to helium, $ε=0.007$. More specifically, $f_{BH}$ is predicted to be $0.3ε-0.5ε$. Based on the present model for BH growth, a scenario for quasar formation is addressed in relation to ultraluminous infrared galaxies.

astro-ph↗

arXiv2001

The Stellar IMF in Very Metal-Deficient Gas

In the context of the star formation through the fragmentation of an extremely metal-deficient protogalactic cloud, the gravitational collapse of filamentary gas clouds is explored with H$_2$ and HD chemistry. It is found by 1D hydrodynamical simulations that the cloud evolution is prescribed mainly by the initial density ($n_0$) and H$_2$ abundance ($x_{\rm H_2,0}$). In particular, it turns out that the evolution of low-density filaments ($n_0 \lesssim 10^5$ cm$^{-3}$) bifurcates at a critical H$_2$ abundance of $x_{\rm H_2,cr}\simeq 3\times 10^{-3}$, beyond which HD cooling overwhelms H$_2$ cooling. The numerical results indicate that the stellar IMF is likely to be double-peaked and deficient in sub-solar mass stars, where the high mass peak of the IMF is around $10M_\odot$ or $10^2M_\odot$, dependently on the initial density and H$_2$ abundance. If the gas in protogalactic clouds is photoionized by UV radiation or shock-heated, the H$_2$ abundance could exceed $x_{\rm H_2,cr}\simeq 3\times 10^{-3}$ by H$^-$ reactions. Then, the high mass peak would be $O(10) M_\odot$.

astro-ph↗

arXiv2001

Formation of Obscuring Walls by Radiation Force from Circumnuclear Starbursts and Implications for Starburst-Active Galactic Nucleus Connection

We explore the formation of dusty gas walls induced by a circumnuclear starburst around an AGN. We concentrate our attention on the role of the radiation force by a starburst as well as an AGN, where the effects of optical depth of dusty gas are taken into consideration. In two-dimensional axisymmetric space, we analyze the configuration and the stability of geometrically thin walls which are in balance between radiation pressure and gravity. As a result, it is shown that the radiation force by the circumnuclear starburst works to stabilize optically thick walls surrounding the nucleus. In the case of a brighter starburst with a fainter AGN, there form double walls, an inner one of which is located between the nucleus and the circumnuclear starburst, and an outer one of which enshrouds both the starburst regions and the nucleus. The total extinction (Av) of both walls turns out to be ~10 for a brighter starburst. As a consequence, double walls could heavily obscure the nucleus to make the AGN type 2. The outer wall may provide an explanation for the recent indications for large-scale obscuring materials in Seyfert 2's. Also, it is predicted that the AGN type is shifts from type 2 to type 1 in several times 10^7 yr according to the stellar evolution in the starburst. In contrast, if the AGN itself is much brighter than the starburst as a quasar is, then neither wall forms regardless of the starburst activity and the nucleus is likely to be identified as type 1. To conclude, the radiatively-supported gas walls could be responsible for the putative correlation between AGN type and the starbursts, whereby Seyfert 2 galaxies are more frequently associated with circumnuclear starbursts than type 1, whereas quasars are mostly observed as type 1 regardless of star-forming activity in the host galaxies.

astro-ph↗

arXiv2001

Circumnuclear obscuration of the Circinus galaxy by a starburst-radiation supported wall

We consider the radiation-hydrodynamical formation of a dusty wall in the circumnuclear regions of the Circinus Seyfert 2 galaxy. We focus on the radiative flux force due to the circumnuclear starburst, the nuclear starburst and the active galactic nucleus (AGN), and analyze the equilibrium configuration and stability of the dusty gas in the circumnuclear regions. The mass distributions used to model the gravitational fields are determined by the observed rotation velocities of the stars and of the gas. Moreover, by using the simple stellar evolution in the circumnuclear starburst, the bolometric luminosity of the starburst is estimated as a function of time. As a result, it is shown that the radiation force by the circumnuclear starburst does play an important role to build up a radiatively-supported dusty wall of $\la$ 100 pc, which obscures the circumnuclear regions with $A_V$ of a few magnitudes. It is also found that the age of a circumnuclear starburst when the circumnuclear regions are enshrouded by the dusty wall is constrained to be $\la 10^8$ yr, which is consistent with the age observationally inferred for the starburst, $4 10^7$ yr $-1.5 10^8$ yr.

astro-ph↗

arXiv2000

On the Initial Mass Function of Population III Stars

The collapse and fragmentation of filamentary primordial gas clouds are explored using 1D and 2D hydrodynamical simulations coupled with the nonequilibrium processes of H2 formation. The simulations show that depending upon the initial density,there are two occasions for the fragmentation of primordial filaments. If a filament has relatively low initial density, the radial contraction is slow due to less effective H2 cooling. This filament tends to fragment into dense clumps before the central density reaches $10^{8-9}$ cm$^{-3}$, where H2 cooling by three-body reactions is effective and the fragment mass is more massive than some tens $M_\odot$. In contrast, if a filament is initially dense, the more effective H2 cooling with the help of three-body reactions allows the filament to contract up to $n\sim 10^{12}$ cm$^{-3}$. After the density reaches $n\sim 10^{12}$ cm$^{-3}$, the filament becomes optically thick to H2 lines and the radial contraction subsequently almost stops. At this final hydrostatic stage, the fragment mass is lowered down to $\approx 1M_\odot$ because of the high density of the filament. The dependence of the fragment mass upon the initial density could be translated into the dependence on the local amplitude of random Gaussian density fields or the epoch of the collapse of a parent cloud. Hence, it is predicted that the initial mass function of Population III stars is likely to be bimodal with peaks of $\approx 10^2 M_\odot$ and $\approx 1M_\odot$, where the relative heights could be a function of the collapse epoch.

astro-ph↗

arXiv2000

UV Background-Induced Bifurcation of the Galactic Morphology

Based upon a novel paradigm of the galaxy formation under UV background, the evolutionary bifurcation of pregalactic clouds is confronted with observations on elliptical and spiral galaxies. The theory predicts that the dichotomy between the dissipational and dissipationless galaxy formation stems from the degree of self-shielding from the UV background radiation. This is demonstrated on a bifurcation diagram of collapse epochs versus masses of pregalactic clouds. Using the observed properties, the collapse epochs are assessed for each type of galaxies with attentive mass estimation. By the direct comparison of the theory with the observations, it turns out that the theoretical bifurcation branch successfully discriminates between elliptical and spiral galaxies. This suggests that the UV background radiation could play a profound role for the differentiation of the galactic morphology into the Hubble sequence.

astro-ph↗