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91探花
Black Hole

Lensing of space time around a black hole. At 91探花 we study black holes observationally and theoretically on all size and time scales - it is some of our core work.

Credit: ALAIN RIAZUELO, IAP/UPMC/CNRS. CLICK HERE TO VIEW MORE IMAGES.

Dr Imogen Whittam

Hintze Fellow

Research theme

  • Astronomy and astrophysics

Sub department

  • Astrophysics

Research groups

  • Galaxy formation and evolution
  • Hintze Centre for Astrophysical Surveys
  • MeerKAT
  • Rubin-LSST
  • The Square Kilometre Array (SKA)
  • Euclid
imogen.whittam@physics.ox.ac.uk
Denys Wilkinson Building, room 558
  • About
  • Publications

Radio spectral properties of star-forming galaxies in the MIGHTEE-COSMOS field and their impact on the far-infrared-radio correlation

Monthly Notices of the Royal Astronomical Society 91探花 University Press 507:256 (2021) 2643-2658

Authors:

Fangxia An, M Vaccari, Ian Smail, Mj Jarvis, Ih Whittam, Cl Hale, S Jin, Jd Collier, E Daddi, J Delhaize, B Frank, Ej Murphy, M Prescott, S Sekhar, Ar Taylor, Y Ao, K Knowles, L Marchetti, Sm Randriamampandry, Z Randriamanakoto

Abstract:

We study the radio spectral properties of 2094 star-forming galaxies (SFGs) by combining our early science data from the MeerKAT International GHz Tiered Extragalactic Exploration (MIGHTEE) survey with VLA, GMRT radio data, and rich ancillary data in the COSMOS field. These SFGs are selected at VLA 3鈥塆Hz, and their flux densities from MeerKAT 1.3鈥塆Hz and GMRT 325鈥塎Hz imaging data are extracted using the 鈥榮uperdeblending鈥 technique. The median radio spectral index is 伪3GHz1.3GHz=鈭0.80卤0.01 without significant variation across the rest-frame frequencies 鈭1.3鈥10鈥塆Hz, indicating radio spectra dominated by synchrotron radiation. On average, the radio spectrum at observer-frame 1.3鈥3鈥塆Hz slightly steepens with increasing stellar mass with a linear fitted slope of 尾 = 鈭0.08 卤 0.01, which could be explained by age-related synchrotron losses. Due to the sensitivity of GMRT 325鈥塎Hz data, we apply a further flux density cut at 3鈥塆Hz (鈦燬3GHz鈮50渭Jy) and obtain a sample of 166 SFGs with measured flux densities at 325鈥塎Hz, 1.3鈥塆Hz, and 3鈥塆Hz. On average, the radio spectrum of SFGs flattens at low frequency with the median spectral indices of 伪1.3GHz325MHz=鈭0.59+0.02鈭0.03 and 伪3.0GHz1.3GHz=鈭0.74+0.01鈭0.02鈦. At low frequency, our stacking analyses show that the radio spectrum also slightly steepens with increasing stellar mass. By comparing the far-infrared-radio correlations of SFGs based on different radio spectral indices, we find that adopting 伪3GHz1.3GHz for k-corrections will significantly underestimate the infrared-to-radio luminosity ratio (qIR) for >17 per cent of the SFGs with measured flux density at the three radio frequencies in our sample, because their radio spectra are significantly flatter at low frequency (0.33鈥1.3鈥塆Hz).

Radio spectral properties of star-forming galaxies in the MIGHTEE-COSMOS field and their impact on the far-infrared-radio correlation

(2021)

Authors:

Fangxia An, M Vaccari, Ian Smail, MJ Jarvis, IH Whittam, CL Hale, S Jin, JD Collier, E Daddi, J Delhaize, B Frank, EJ Murphy, M Prescott, S Sekhar, AR Taylor, Y Ao, K Knowles, L Marchetti, SM Randriamampandry, Z Randriamanakoto

The infrared-radio correlation of star-forming galaxies is strongly M-star-dependent but nearly redshift-invariant since z similar to 4

Astronomy and Astrophysics European Southern Observatory 647 (2021) A123

Authors:

I Delvecchio, E Daddi, Mt Sargent, Matt Jarvis, D Elbaz, S Jin, D Liu, Imogen Whittam, H Algera, R Carraro, C D'Eugenio, J Delhaize, Bs Kalita, S Leslie, D Cs Molnar, M Novak, I Prandoni, V Smolcic, Y Ao, M Aravena, F Bournaud, Jd Collier, Sm Randriamampandry, Z Randriamanakoto, G Rodighiero, J Schober, Sv White, G Zamorani

Abstract:

Over the past decade, several works have used the ratio between total (rest 8鈭1000 渭m) infrared and radio (rest 1.4 GHz) luminosity in star-forming galaxies (qIR), often referred to as the infrared-radio correlation (IRRC), to calibrate the radio emission as a star formation rate (SFR) indicator. Previous studies constrained the evolution of qIR with redshift, finding a mild but significant decline that is yet to be understood. Here, for the first time, we calibrate qIR as a function of both stellar mass (M鈰) and redshift, starting from an M鈰-selected sample of > 400 000 star-forming galaxies in the COSMOS field, identified via (NUV鈥呪垝鈥卹)/(r鈥呪垝鈥匤) colours, at redshifts of 0.1鈥<鈥剒鈥<鈥4.5. Within each (M鈰,z) bin, we stacked the deepest available infrared/sub-mm and radio images. We fit the stacked IR spectral energy distributions with typical star-forming galaxy and IR-AGN templates. We then carefully removed the radio AGN candidates via a recursive approach. We find that the IRRC evolves primarily with M鈰, with more massive galaxies displaying a systematically lower qIR. A secondary, weaker dependence on redshift is also observed. The best-fit analytical expression is the following: qIR(M鈰,鈥唞) = (2.646 卤 0.024) 脳 (1鈥+鈥厇)(鈥呪垝鈥0.023鈥吢扁0.008)鈥(0.148 卤 0.013) 脳 (log鈥哅鈰/M鈯欌呪垝鈥10). Adding the UV dust-uncorrected contribution to the IR as a proxy for the total SFR would further steepen the qIR dependence on M鈰. We interpret the apparent redshift decline reported in previous works as due to low-M鈰 galaxies being progressively under-represented at high redshift, as a consequence of binning only in redshift and using either infrared or radio-detected samples. The lower IR/radio ratios seen in more massive galaxies are well described by their higher observed SFR surface densities. Our findings highlight the fact that using radio-synchrotron emission as a proxy for SFR requires novel M鈰-dependent recipes that will enable us to convert detections from future ultra-deep radio surveys into accurate SFR measurements down to low-M鈰 galaxies with low SFR.

MIGHTEE: are giant radio galaxies more common than we thought?

MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY 501:3 (2021) 3833-3845

Authors:

J Delhaize, I Heywood, M Prescott, Mj Jarvis, I Delvecchio, Ih Whittam, Sv White, Mj Hardcastle, Cl Hale, J Afonso, Y Ao, M Brienza, M Brueggen, Jd Collier, E Daddi, M Glowacki, N Maddox, Lk Morabito, I Prandoni, Z Randriamanakoto, S Sekhar, Fangxia An, Nj Adams, S Blyth, Raa Bowler, L Leeuw, L Marchetti, Sm Randriamampandry, K Thorat, N Seymour, O Smirnov, Ar Taylor, C Tasse, M Vaccari

MIGHTEE: are giant radio galaxies more common than we thought?

Monthly Notices of the Royal Astronomical Society 91探花 University Press 501:3 (2020) 3833-3845

Authors:

J Delhaize, Ian Heywood, M Prescott, Matthew Jarvis, I Delvecchio, Ih Whittam, Sv White, Mj Hardcastle, Cl Hale, J Afonso, Y Ao, M Brienza, M Br眉ggen, Jd Collier, E Daddi, M Glowacki, N Maddox, Lk Morabito, I Prandoni, Z Randriamanakoto, S Sekhar, F An, Nj Adams, S Blyth, Rebecca Bowler, L Leeuw, L Marchetti, Sm Randriamampandry, K Thorat, N Seymour, O Smirnov, Ar Taylor, C Tasse, M Vaccari

Abstract:

We report the discovery of two new giant radio galaxies (GRGs) using the MeerKAT International GHz Tiered Extragalactic Exploration (MIGHTEE) survey. Both GRGs were found within a 鈭1鈥塪eg2 region inside the COSMOS field. They have redshifts of z = 0.1656 and z = 0.3363 and physical sizes of 2.4 and 2.0 Mpc, respectively. Only the cores of these GRGs were clearly visible in previous high-resolution Very Large Array observations, since the diffuse emission of the lobes was resolved out. However, the excellent sensitivity and uv coverage of the new MeerKAT telescope allowed this diffuse emission to be detected. The GRGs occupy an unpopulated region of radio power 鈥 size parameter space. Based on a recent estimate of the GRG number density, the probability of finding two or more GRGs with such large sizes at z < 0.4 in a 鈭1鈥塪eg2 field is only 2.7 脳 10鈭6, assuming Poisson statistics. This 91探花s the hypothesis that the prevalence of GRGs has been significantly underestimated in the past due to limited sensitivity to low surface brightness emission. The two GRGs presented here may be the first of a new population to be revealed through surveys like MIGHTEE that provide exquisite sensitivity to diffuse, extended emission.

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