Masahiro Kawasaki’s research while affiliated with The University of Tokyo and other places

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Publications (316)


EMPRESS. X. Spatially resolved mass-metallicity relation in extremely metal-poor galaxies: evidence of episodic star-formation fueled by a metal-poor gas infall
  • Preprint
  • File available

December 2024

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11 Reads

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Yuki Isobe

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Yechi Zhang

Using the Subaru/FOCAS IFU capability, we examine the spatially resolved relationships between gas-phase metallicity, stellar mass, and star-formation rate surface densities (Sigma_* and Sigma_SFR, respectively) in extremely metal-poor galaxies (EMPGs) in the local universe. Our analysis includes 24 EMPGs, comprising 9,177 spaxels, which span a unique parameter space of local metallicity (12+log(O/H) = 6.9 to 7.9) and stellar mass surface density (Sigma_* ~ 10^5 to 10^7 Msun/kpc^2), extending beyond the range of existing large integral-field spectroscopic surveys. Through spatially resolved emission line diagnostics based on the [NII] BPT-diagram, we verify the absence of evolved active galactic nuclei in these EMPGs. Our findings reveal that, while the resolved mass-metallicity relation exhibits significant scatter in the low-mass regime, this scatter is closely correlated with local star-formation surface density. Specifically, metallicity decreases as Sigma_SFR increases for a given Sigma_*. Notably, half of the EMPGs show a distinct metal-poor horizontal branch on the resolved mass-metallicity relation. This feature typically appears at the peak clump with the highest Sigma_* and Sigma_SFR and is surrounded by a relatively metal-enriched ambient region. These findings support a scenario in which metal-poor gas infall fuels episodic star formation in EMPGs, consistent with the kinematic properties observed in these systems. In addition, we identify four EMPGs with exceptionally low central metallicities (12+log(O/H) <~ 7.2), which display only a metal-poor clump without a surrounding metal-rich region. This suggests that such ultra-low metallicity EMPGs, at less than a few percent of the solar metallicity, may serve as valuable analogs for galaxies in the early stages of galaxy evolution.

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Affleck-Dine leptogenesis scenario for resonant production of sterile neutrino dark matter

August 2024

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1 Read

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3 Citations

Sterile neutrino is a fascinating candidate for dark matter. In this paper, we examine the Affleck-Dine (AD) leptogenesis scenario generating a large lepton asymmetry, which can induce the resonant production of sterile neutrino dark matter via the Shi-Fuller (SF) mechanism. We also revisit the numerical calculation of the SF mechanism and the constraints from current X-ray and Lyman-α forest observations. We find that the AD leptogenesis scenario can explain the production of sterile neutrino dark matter by incorporating a non-topological soliton with a lepton charge called L-ball. Finally, we discuss an enhancement of second-order gravitational waves at the L-ball decay and investigate the testability of our scenario with future gravitational wave observations.


Primordial origin of supermassive black holes from axion bubbles

We study a modification of the primordial black hole (PBH) formation model from axion bubbles. We assume that the Peccei-Quinn scalar rolls down in the radial direction from a large field value to the potential minimum during inflation, which suppresses the axion fluctuations and weakens the clustering of PBHs on large scales. We find that the modified model can produce a sufficient number of PBHs that seed the supermassive black holes while avoiding the observational constraints from isocurvature perturbations and angular correlation of the high-redshift quasars.


Figure 2: Volume fraction of lepton bubbles per ln k for different values of N * . The horizontal axis denotes the bubble size in terms of the wave number. The lepton bubbles on the left side of the black line form PBHs, and those on the right side remain as bubbles. Here, we fixed f PBH = 3 × 10 −9 , c ′ 1 = 1 and c ′ 2 = 0.005. The smaller bubbles have larger volume fractions. The larger N * becomes, the more lepton bubbles remain.
Figure 3: PBH correlation function for different values of N * . Here, we take c ′ 2 = 0.005 and fix f PBH by choosing˜φchoosing˜ choosing˜φ c . The left end has apparent divergence coming from the selfcorrelation at the scale of the PBH-forming bubble. The right end goes to zero at the edge of the observable universe. In the actual numerical calculation, it is difficult to evaluate the correlation near those endpoints. Larger N * provides the suppression of the correlation in a wider range of scales.
Supermassive black hole formation from Affleck-Dine mechanism with suppressed clustering on large scales

May 2024

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15 Reads

We study a primordial black hole (PBH) formation model based on the framework of the inhomogeneous Affleck-Dine (AD) mechanism, which can explain the seeds of supermassive black holes (SMBHs). This model, however, predicts strong clustering of SMBHs that is inconsistent with the observation of angular correlation of quasars. In this paper, we propose a modified model that can significantly reduce the PBH clustering on large scales by considering a time-dependent Hubble-induced mass during inflation. The quasar angular correlation is suppressed by the large Hubble-induced mass in the early stage of inflation while the small Hubble-induced mass in the late stage leads to the AD field fluctuations large enough for PBH formation as in the original model. As a result, the modified scenario can successfully explain the seeds of SMBHs.


FIG. 1. Evolution of the Q-ball charge is shown in the purple arrow. We show the charge at the formation (5), that for the decay at present (8), that when the transformation from the new-type into the gauge-mediation type takes place (11), and that when the decay channel to pions opens (12) as the function of m 3=2 , for ϕ 0 ¼ 0.3M P and jKj ¼ 0.02, in blue, red, magenta, and green lines, respectively.
MeV gamma rays from Q -ball decay

April 2024

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6 Reads

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1 Citation

Physical Review D

We study the supersymmetric Q balls which decay at present and find that they create a distinctive spectrum of gamma rays at around O(10) MeV. The charge of the Q ball is lepton numbers in order for the lifetime to be as long as the present age of the Universe, and the main decay products are light leptons. However, as the charge of the Q ball decreases, the decay channel into pions becomes kinematically allowed towards the end of the decay, and the pions are produced at rest. Immediately, π 0 decays into two photons with the energy of 67.5 MeV, half the pion mass, which exhibits a unique emission line. In addition, π ± decay into μ ± , which further decay with emitting internal bremsstrahlung, whose spectrum has a sharp cutoff at ∼ 50 MeV . If the observations find these peculiar features of the gamma-ray spectrum in the future, it could be a smoking gun of the supersymmetric Q -ball decay at present. Published by the American Physical Society 2024


Axion curvaton model for the gravitational waves observed by pulsar timing arrays

February 2024

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5 Reads

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20 Citations

Physical Review D

The stochastic gravitational wave background (SGWB) recently detected by the PTA collaborations could be the gravitational waves (GWs) induced by curvature perturbations. However, primordial black holes (PBHs) might be overproduced if the SGWB is explained by the GWs induced by the curvature perturbations that follow the Gaussian distribution. This motivates models associated with the non-Gaussianity of the curvature perturbations that suppress the PBH production rate. In this work, we show that the axion curvaton model can produce the curvature perturbations that induce GWs for the detected SGWB while preventing the PBH overproduction with the non-Gaussianity.


Enhancement of gravitational waves at Q-ball decay including non-linear density perturbations

January 2024

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15 Reads

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24 Citations

The existence of a stochastic gravitational wave background is indicated by the recent pulsar timing array (PTA) experiments. We study the enhanced production of second-order gravitational waves from the scalar perturbations when the universe experiences a transition from the early matter-dominated era to the radiation-dominated era due to Q-ball decay. We extend the analysis in previous work by including the frequency range where density perturbations go non-linear and find that the resultant gravitational wave spectrum can be consistent with that favored by the recent PTA experiment results.


Figure 1. (a) From left to right: SDSS cutout, Hα flux map, line-of-sight velocity map, and velocity dispersion map for each EMPG whose high-resolution data is reported in this study and Paper IX. Spaxels with S/N (Hα) >3 are plotted. The red rectangle on the SDSS cutout indicates the pointing position of our IFU observations while the arrow indicates the direction of the x-axis. The x-and y-axes are presented in arcsec. The black contours represent the Hα flux in the range of ( ) = -a --F log erg s cm 17 H 1 2 to −14.5 with a step of 0.5 dex. The red circles highlight the apertures we obtained by source detection (see Section 2.4). Within the apertures, we fit disk rotation models. (b) The global Toomre Q parameter as a function of M * (left) and metallicity (right). The red triangles indicate the four EMPGs with large global Toomre Q values that are out of the y-axis range. All of the EMPGs shown in this plot have Q > 1.
Figure 1. (Continued.)
Figure 2. (Top) s v max 0 as a function of stellar mass (left) and gas-phase metallicity (right). The red squares represent individual EMPGs while the red circles represent average values in stellar mass (metallicity) bins. The gray circles and triangles indicate data taken from the DYNAMO survey (Green et al. 2014) and the SHαDE survey (Barat et al. 2020), respectively. (Bottom) Same as the top panels but for f gas . We plot the median values with red circles. The gray regions in the bottom-left panel indicate the observational limit for f gas (see Section 3.1).
Figure 3. Same as the top-right panel of Figure 2 but color coded by the categories given by K. Nakajima et al. (2023, in preparation). The y-axis is changed to linear scale. Category A EMPGs have surrounding metal-enriched regions that may have come from older stellar populations, while Category B EMPGs only show metal-poor regions given by the recent star formation. Category C EMPGs are possibly in a transition stage.
Figure 4. Enclosed mass profiles. The red, yellow, cyan, and black curves represent dynamical, stellar, gas, and DM mass profiles, respectively. The vertical dotted lines show the effective radius of Hα. The edge of the plots corresponds to the outermost radii used for the kinematic analysis.
EMPRESS. XII. Statistics on the Dynamics and Gas Mass Fraction of Extremely Metal-poor Galaxies

January 2024

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64 Reads

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3 Citations

The Astrophysical Journal

We present the demography of the dynamics and gas mass fraction of 33 extremely metal-poor galaxies (EMPGs) with metallicities of 0.015–0.195 Z ⊙ and low stellar masses of 10 ⁴ –10 ⁸ M ⊙ in the local universe. We conduct deep optical integral field spectroscopy (IFS) for the low-mass EMPGs with the medium-high resolution ( R = 7500) grism of the 8 m Subaru FOCAS IFU instrument by the EMPRESS 3D survey, and investigate the H α emission of the EMPGs. Exploiting the resolution high enough for the low-mass galaxies, we derive gas dynamics with the H α lines by the fitting of three-dimensional disk models. We obtain an average maximum rotation velocity ( v rot ) of 15 ± 3 km s ⁻¹ and an average intrinsic velocity dispersion ( σ 0 ) of 27 ± 10 km s ⁻¹ for 15 spatially resolved EMPGs out of 33 EMPGs, and find that all 15 EMPGs have v rot / σ 0 < 1 suggesting dispersion-dominated systems. There is a clear decreasing trend of v rot / σ 0 with the decreasing stellar mass and metallicity. We derive the gas mass fraction ( f gas ) for all 33 EMPGs, and find no clear dependence on stellar mass and metallicity. These v rot / σ 0 and f gas trends should be compared with young high- z galaxies observed by the forthcoming JWST IFS programs to understand the physical origins of the EMPGs in the local universe.


Hill-top inflation from Dai-Freed anomaly in the standard model — a solution to the iso-curvature problem of the axion dark matter

January 2024

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5 Reads

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1 Citation

The discrete symmetry Z 4 in the standard model (SM) with three right-handed neutrinos is free from the Dai-Freed anomaly. Motivated by this Z 4 symmetry, we constructed a topological inflation model consistent with all known constraints and observations. However, we assumed a specific inflaton potential in the previous work. In this paper we extend the inflaton potential in a more general form allowed by the discrete Z 4 gauge symmetry and show that consistent hilltop inflation is realized.We find that the Hubble parameter H_inf can be smaller than ≃ 10⁹ GeV so that the isocurvature fluctuations of the axion dark matter are sufficiently suppressed. Furthermore, the running of the spectral index can be as large as dns /ln k ≃ 0.0018 which will be tested in future CMB observations. Since this discrete Z 4 acts on the SM, the inflaton can couple to pairs of the right-handed neutrinos and hence the reheating temperature can be high as ∼ 10¹⁰ GeV, producing the cosmic baryon asymmetry naturally through the thermal leptogenesis.


Figure 1. Spectral index as a function of g for N * = 50 − 60. The observed value with 1σ and 2σ errors is shown by the magenta-shaded region.
χ N for N = 50, 55 and 60.
Dai-Freed anomaly in the standard model and topological inflation

November 2023

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5 Reads

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3 Citations

Journal of High Energy Physics

A bstract When we impose discrete symmetries in the standard model we have Dai-Freed global anomalies. However, interestingly if we introduce three right-handed neutrinos we can have an anomaly-free discrete Z 4 gauge symmetry. This Z 4 symmetry should be spontaneously broken down to the Z 2 symmetry to generate the heavy Majorana masses for the right-handed neutrinos. We show that this symmetry breaking naturally generates topological inflation, which is consistent with the CMB observations at present and predicts a significant tensor mode with scalar-tensor ratio r > 0 . 03. The right-handed neutrinos play an important role in reheating processes. The reheating temperature is as high as ∼ 10 ⁸ GeV, and non-thermal leptogenesis successfully takes place.


Citations (55)


... Furthermore, the out-of-equilibrium decay of the ν c i 's, which are produced during reheating, provides us with an explanation of the observed baryon asymmetry of the universe (BAU) [59] via non-thermal leptogenesis (nTL) [60][61][62]. Consistency of the BAU, gravitino ( G) constraint [63,64] and the neutrino data [65] can be achieved in regions of the parameter space with low r values. Also, taking advantage of the adopted R symmetry, the parameter µ appearing in the mixing term between the two electroweak Higgs fields in the superpotential of the Minimal SUSY Standard Model (MSSM) can be explained as in refs. ...

Reference:

T-model Higgs inflation and metastable cosmic strings
Revisiting Big-Bang Nucleosynthesis Constraints on Long-Lived Decaying Particles
  • Citing Preprint
  • September 2017

... It was discussed in [18] that a large asymmetry of the active neutrinos can be generated due to the Affleck-Dine mechanism and Q-ball decay. Then the RHN (or sterile neutrino) DM (see refs. ...

Affleck-Dine leptogenesis scenario for resonant production of sterile neutrino dark matter

... Another possibility is to make use of the large isocurvature perturbations of baryons or dark matter. For instance, PBH formation from collapsing baryon/axion bubbles represents an interesting realization of such a mechanism [16][17][18][19][20][21][22][23][24]. ...

Primordial origin of supermassive black holes from axion bubbles

... Many theoretical frameworks of the early universe predict an enhancement of curvature perturbations on small scales, leading to the generation of SIGWs with distinctive signatures. These predictions stem from scenarios such as single-field inflation with ultra-slow-roll phases [7][8][9][10][11][12][13][14][15][16][17][18][19][20][21][22], multifield dynamics [23][24][25][26][27][28][29] and curvaton models [30][31][32][33][34][35][36][37][38][39][40][41]. The detection and characterization of SIGWs would provide direct insight into the processes shaping the primordial universe. ...

Axion curvaton model for the gravitational waves observed by pulsar timing arrays
  • Citing Article
  • February 2024

Physical Review D

... However, GW production will continue in the nonlinear regime (see, e.g. Ref. [96] for early analytical approximations and Ref. [97] for a numerical simulation in a gradual transition). For this reason, we take k cut as an arbitrary value between k NL ≤ k cut ≤ k uv (beyond k uv it is difficult to talk about fluctuations in the PBH-dominated universe). ...

Enhancement of gravitational waves at Q-ball decay including non-linear density perturbations

... The project encompasses diverse investigations, including the search for rare metal-poor systems and their global properties (Kojima et al. 2020;Nishigaki et al. 2023), the study of chemical abundances to trace past massive star formation and explosion (Kojima et al. 2021;Isobe et al. 2022;Watanabe et al. 2024), and the examination of ionizing spectra to infer the presence of intermediate-mass black holes (Umeda et al. 2022;Hatano et al. 2023Hatano et al. , 2024. Furthermore, EMPRESS examines the dynamics and outflows of EMPGs to explore gas properties and feedback mechanisms Xu et al. 2022Xu et al. , 2024 and delves into primordial abundances as a direct test of Big Bang nucleosynthesis models (Matsumoto et al. 2022; see also Kawasaki & Murai 2022). In this study, we aim to map the metallicity distribution within these galaxies by utilizing the 3D datacubes of EMPGs, focusing on how stellar mass and star formation activity shape the local chemical enrichment processes. ...

EMPRESS. XII. Statistics on the Dynamics and Gas Mass Fraction of Extremely Metal-poor Galaxies

The Astrophysical Journal

... It is very much welcome since we can control the inflaton potential to generate consistent inflation by the discrete symmetry. In fact, we constructed a topological inflation model based on the discrete Z 4 symmetry which is consistent with all present observations [7]. However, this model predicts the Hubble parameter during inflation, H inf ≃ 10 12 GeV which causes too large isocurvature fluctuations of the axion dark matter. ...

Dai-Freed anomaly in the standard model and topological inflation

Journal of High Energy Physics

... Another possibility is to make use of the large isocurvature perturbations of baryons or dark matter. For instance, PBH formation from collapsing baryon/axion bubbles represents an interesting realization of such a mechanism [16][17][18][19][20][21][22][23][24]. ...

Clustering of primordial black holes from QCD axion bubbles

... 2. EMPRESS 3D DATA 2.1. Sample As presented in part by Isobe et al. (2023) and Xu et al. (2024) (see also Kashiwagi et al. 2021 as a pilot study), our target sample for the FOCAS IFU spectroscopy is derived from the compilation of local metal-poor galaxies provided in . This comprehensive catalog includes 103 EMPGs with 12 + log(O/H) ≤ 7.69, alongside 82 moderately metalpoor galaxies with 7.69 < 12 + log(O/H) ≲ 8.1. ...

EMPRESS. IX. Extremely Metal-poor Galaxies are Very Gas-rich Dispersion-dominated Systems: Will the James Webb Space Telescope Witness Gaseous Turbulent High-z Primordial Galaxies?

The Astrophysical Journal