5 research outputs found

    MIGHTEE-HI: the HI Size-Mass relation over the last billion years

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    We present the observed HI size-mass relation of 204204 galaxies from the MIGHTEE Survey Early Science data. The high sensitivity of MeerKAT allows us to detect galaxies spanning more than 4 orders of magnitude in HI mass, ranging from dwarf galaxies to massive spirals, and including all morphological types. This is the first time the relation has been explored on a blind homogeneous data set which extends over a previously unexplored redshift range of 0<z<0.0840 < z < 0.084, i.e. a period of around one billion years in cosmic time. The sample follows the same tight logarithmic relation derived from previous work, between the diameter (DHID_{\rm HI}) and the mass (MHIM_{\rm HI}) of HI discs. We measure a slope of 0.501±0.0080.501\pm 0.008, an intercept of 3.2520.074+0.073-3.252^{+0.073}_{-0.074}, and an observed scatter of 0.0570.057 dex. For the first time, we quantify the intrinsic scatter of 0.054±0.0030.054 \pm 0.003 dex (10%{\sim} 10 \%), which provides a constraint for cosmological simulations of galaxy formation and evolution. We derive the relation as a function of galaxy type and find that their intrinsic scatters and slopes are consistent within the errors. We also calculate the DHIMHID_{\rm HI} - M_{\rm HI} relation for two redshift bins and do not find any evidence for evolution with redshift. These results suggest that over a period of one billion years in lookback time, galaxy discs have not undergone significant evolution in their gas distribution and mean surface mass density, indicating a lack of dependence on both morphological type and redshift.Comment: 10 pages, 5 figures, accepted for publication in MNRA

    MIGHTEE-HI: The first MeerKAT HI mass function from an untargeted interferometric survey

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    We present the first measurement of the HI mass function (HIMF) using data from MeerKAT, based on 276 direct detections from the MIGHTEE Survey Early Science data covering a period of approximately a billion years (0z0.0840 \leq z \leq 0.084 ). This is the first HIMF measured using interferometric data over non-group or cluster field, i.e. a deep blank field. We constrain the parameters of the Schechter function which describes the HIMF with two different methods: 1/Vmax1/\rm V_{\rm max} and Modified Maximum Likelihood (MML). We find a low-mass slope α=1.290.26+0.37\alpha=-1.29^{+0.37}_{-0.26}, `knee' mass log10(M/M)=10.070.24+0.24\log_{10}(M_{*}/{\rm M_{\odot}}) = 10.07^{+0.24}_{-0.24} and normalisation log10(ϕ/Mpc3)=2.340.36+0.32\log_{10}(\phi_{*}/\rm Mpc^{-3})=-2.34^{+0.32}_{-0.36} (H0=67.4H_0 = 67.4 kms1^{-1} Mpc1^{-1}) for 1/Vmax1/\rm V_{\rm max} and α=1.440.10+0.13\alpha=-1.44^{+0.13}_{-0.10}, `knee' mass log10(M/M)=10.220.13+0.10\log_{10}(M_{*}/{\rm M_{\odot}}) = 10.22^{+0.10}_{-0.13} and normalisation log10(ϕ/Mpc3)=2.520.14+0.19\log_{10}(\phi_{*}/\rm Mpc^{-3})=-2.52^{+0.19}_{-0.14} for MML. When using 1/Vmax1/\rm V_{\rm max} we find both the low-mass slope and `knee' mass to be consistent within 1σ1\sigma with previous studies based on single-dish surveys. The cosmological mass density of HI is found to be slightly larger than previously reported: ΩHI=5.460.99+0.94×104h67.41\Omega_{\rm HI}=5.46^{+0.94}_{-0.99} \times 10^{-4}h^{-1}_{67.4} from 1/Vmax1/\rm V_{\rm max} and ΩHI=6.310.31+0.31×104h67.41\Omega_{\rm HI}=6.31^{+0.31}_{-0.31} \times 10^{-4}h^{-1}_{67.4} from MML but consistent within the uncertainties. We find no evidence for evolution of the HIMF over the last billion years.Comment: 13 pages, 9 figures, accepted for publication in MNRA

    MIGHTEE-Hi: Evolution of Hi Scaling Relations of Star-forming Galaxies at z &lt; 0.5*

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    We present the first measurements of H I galaxy scaling relations from a blind survey at z > 0.15. We perform spectral stacking of 9023 spectra of star-forming galaxies undetected in H I at 0.23 < z < 0.49, extracted from MIGHTEE-H I Early Science data cubes, acquired with the MeerKAT radio telescope. We stack galaxies in bins of galaxy properties (stellar mass M *, star formation rateSFR, and specific star formation rate sSFR, with sSFR ≡ M */SFR), obtaining ≳5σ detections in most cases, the strongest H I-stacking detections to date in this redshift range. With these detections, we are able to measure scaling relations in the probed redshift interval, finding evidence for a moderate evolution from the median redshift of our sample z med ~ 0.37 to z ~ 0. In particular, low-M * galaxies ( {\mathrm{log}}_{10}({M}_{* }/{M}_{\odot })\sim 9 )experienceastrongHIdepletion( 0.5dexinlog10(MHI/M⊙) ), while massive galaxies ( {\mathrm{log}}_{10}({M}_{* }/{M}_{\odot })\sim 11$ ) keep their H I mass nearly unchanged. When looking at the star formation activity, highly star-forming galaxies evolve significantly in M H I (f H I, where f H I ≡ M H I/M *) at fixed SFR (sSFR), while at the lowest probed SFR (sSFR) the scaling relations show no evolution. These findings suggest a scenario in which low-M * galaxies have experienced a strong H I depletion during the last ~5 Gyr, while massive galaxies have undergone a significant H I replenishment through some accretion mechanism, possibly minor mergers. Interestingly, our results are in good agreement with the predictions of the SIMBA simulation. We conclude that this work sets novel important observational constraints on galaxy scaling relations

    MIGHTEE-H\u2009i: the baryonic Tully\u2013Fisher relation over the last billion years

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    Using a sample of 67 galaxies from the MeerKAT International GigaHertz Tiered Extragalactic Exploration Survey Early Science data, we study the H\u2009i-based baryonic Tully\u2013Fisher relation (bTFr), covering a period of 3c1 billion years (0 64 z 64 0.081). We consider the bTFr based on two different rotational velocity measures: the width of the global H\u2009i profile and Vout, measured as the outermost rotational velocity from the resolved H\u2009i rotation curves. Both relations exhibit very low intrinsic scatter orthogonal to the best-fitting relation (\u3c3 a5 = 0.07 \ub1 0.01), comparable to the SPARC sample at z 43 0. The slopes of the relations are similar and consistent with the z 43 0 studies (\u20603.66+0.35 120.29 for W50 and 3.47+0.37 120.30 for Vout). We find no evidence that the bTFr has evolved over the last billion years, and all galaxies in our sample are consistent with the same relation independent of redshift and the rotational velocity measure. Our results set-up a reference for all future studies of the H\u2009i-based bTFr as a function of redshift that will be conducted with the ongoing deep SKA pathfinders surveys

    MIGHTEE-HI: The MHIMM_{\rm HI}-M_{\star} relation over the last billion years

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    We measure the MHIMM_{\rm HI}-M_{\star} relation over the last billion years down to MHI107MM_{\rm HI}\sim 10^7 M_{\odot} using the MIGHTEE Early Science data with a Bayesian technique. This technique is applied to the HI detections, without binning the datasets, while taking account of the intrinsic scatter in the MHIMM_{\rm HI}-M_{\star} relation. We divide the full sample of 249 galaxies into 161 spirals, 64 irregulars, 15 mergers, and 9 elliptical galaxies to measure their MHIMM_{\rm HI}-M_{\star} relations. We fit this relation with both linear and non-linear models, and find that the non-linear model is preferred over the linear one for the full HI-selected sample with a measured transition stellar mass of log10(M\log_{10}(M_\star/M)M_{\odot}) = 9.150.95+0.89.15^{+0.8}_{-0.95}, beyond which the measured slope flattens. This finding supports the view that the lack of HI gas is ultimately responsible for the decreasing star formation rate observed in the massive main sequence galaxies. For the spiral galaxies alone, which are biased towards those galaxies with the highest stellar masses in our sample, the slope beyond the transition mass is shallower than for the full sample, indicative of distinct gas processes ongoing for the spirals/high-mass galaxies from other types of galaxies with lower stellar masses. We also observe a moderate evolution of the MHIMM_{\rm HI}-M_{\star} relation when splitting our samples into two redshift bins over the last billion years, which can largely be attributed to the effect of sample selection and hence highlights the potential of the full MIGHTEE survey.Comment: 14 pages, submitted to MNRA
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