2020MNRAS.492.4927K


Query : 2020MNRAS.492.4927K

2020MNRAS.492.4927K - Mon. Not. R. Astron. Soc., 492, 4927-4944 (2020/March-2)

An ALMA survey of the SCUBA-2 cosmology legacy survey UKIDSS/UDS field: Dust attenuation in high-redshift Lyman-break galaxies.

KOPROWSKI M.P., COPPIN K.E.K., GEACH J.E., DUDZEVICIUTE U., SMAIL I., ALMAINI O., AN F., BLAIN A.W., CHAPMAN S.C., CHEN C.-C., CONSELICE C.J., DUNLOP J.S., FARRAH D., GULLBERG B., HARTLEY W., IVISON R.J., KARSKA A., MALTBY D., MALEK K., MICHALOWSKI M.J., POPE A., SALIM S., SCOTT D., SIMPSON C.J., SIMPSON J.M., SWINBANK A.M., THOMSON A.P., WARDLOW J.L., VAN DER WERF P.P. and WHITAKER K.E.

Abstract (from CDS):

We analyse 870 µm Atacama Large Millimetre Array (ALMA) dust continuum detections of 41 canonically selected z ≃ 3 Lyman-break galaxies (LBGs), as well as 209 ALMA-undetected LBGs, in follow-up of SCUBA-2 mapping of the UKIDSS Ultra Deep Survey (UDS) field. We find that our ALMA-bright LBGs lie significantly off the local IRX-beta relation and have relatively bluer rest-frame UV slopes (as parametrized by β), given their high values of the `infrared excess' (IRX ≡ LIR/LUV), relative to the average `local' IRX-β relation. We attribute this finding in part to the young ages of the underlying stellar populations but we find that the main reason behind the unusually blue UV slopes are the relatively shallow slopes of the corresponding dust attenuation curves. We show that, when stellar masses, M*, are being established via SED fitting, it is absolutely crucial to allow the attenuation curves to vary (rather than fixing it on Calzetti-like law), where we find that the inappropriate curves may underestimate the resulting stellar masses by a factor of ≃2-3x on average. In addition, we find these LBGs to have relatively high specific star-formation rates (sSFRs), dominated by the dust component, as quantified via the fraction of obscured star formation (f_obs≡ {SFRIR/SFRUV+IR}). We conclude that the ALMA-bright LBGs are, by selection, massive galaxies undergoing a burst of a star formation (large sSFRs, driven, for example, by secular or merger processes), with a likely geometrical disconnection of the dust and stars, responsible for producing shallow dust attenuation curves.

Abstract Copyright: © 2020 The Author(s) Published by Oxford University Press on behalf of the Royal Astronomical Society

Journal keyword(s): dust - extinction - galaxies: evolution - galaxies: high-redshift - galaxies: ISM - galaxies: star formation - cosmology: observations

Simbad objects: 41

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Number of rows : 41
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 AS2UDS 0678.0 G 02 16 02.6253504 -04 49 41.760002   27.41088 23.864 26.67593   ~ 3 0
2 AS2UDS 0436.0 G 02 16 09.555596 -04 55 50.91788     25.0525 26.84856   ~ 3 0
3 AS2UDS J021611.71-050053.65 rG 02 16 11.72 -05 00 54.0   27.27005 22.2926 25.31193   ~ 6 0
4 AS2UDS 0573.0 QSO 02 16 16.8154637 -05 12 53.812496   23.67928 21.5744 23.09501   ~ 7 0
5 AS2UDS 0300.0 G 02 16 19.7268826 -04 50 41.368641   27.47083 23.3911 26.09685   ~ 3 0
6 AS2UDS 0004.0 G 02 16 47.93 -05 01 29.9     22.2537 26.76636   ~ 7 0
7 AS2UDS 0596.0 G 02 17 02.4461726 -04 52 34.361142     23.9974 26.92317   ~ 3 0
8 AS2UDS 0162.1 G 02 17 03.8516 -05 15 54.237   28.407 23.9956 26.19350   ~ 7 0
9 AS2UDS 0228.0 G 02 17 04.7407846 -04 39 39.981525   26.00717 25.27003 25.06844   ~ 3 0
10 AS2UDS 0086.0 G 02 17 19.7728903 -04 48 55.816763     24.0218 25.51139   ~ 3 0
11 AS2UDS 0308.0 G 02 17 21.8234 -05 14 25.876     23.0863 26.09378   ~ 8 0
12 AS2UDS 0481.1 G 02 17 33.4221197 -04 47 23.864325     24.5359 27.11630   ~ 3 0
13 AS2UDS 0278.0 AGN 02 17 35.593 -04 42 59.83   26.22 22.2482 25.13624   ~ 6 0
14 AS2UDS 0480.0 G 02 17 36.1378925 -04 55 51.214047   27.37660 24.7386 26.80082   ~ 3 0
15 AS2UDS 0099.0 G 02 17 37.24 -04 47 53.0   27.89188 22.9821 26.55641   ~ 4 0
16 AS2UDS 0403.0 G 02 17 41.2569924 -05 32 14.458255   28.03166 24.1513 26.89902   ~ 3 0
17 AS2UDS J021744.26-052008.59 EmG 02 17 44.27 -05 20 08.6     22.7521 26.05094   ~ 13 0
18 AS2UDS 0266.0 G 02 17 51.77582 -05 09 50.4224   28.02670 22.5852 26.66624   ~ 8 0
19 AS2UDS 0044.0 G 02 17 54.80 -05 23 23.0   27.54170 22.9207 26.76316   ~ 7 0
20 AS2UDS 0441.0 G 02 17 57.7309678 -05 06 36.968540     23.4379 26.99696   ~ 4 0
21 AS2UDS 0008.0 G 02 18 03.01 -05 28 41.9     23.9648 26.79586   ~ 7 0
22 AS2UDS 0583.0 G 02 18 03.8491 -05 12 39.824   25.67462 22.8528 25.01980   ~ 5 0
23 AS2UDS 0006.0 G 02 18 05.65 -05 10 49.7     24.3077 26.78275   ~ 9 0
24 AS2UDS 0485.0 G 02 18 08.1234718 -05 31 25.415585   25.94410 21.6815 25.12228   ~ 3 0
25 AS2UDS 0514.0 G 02 18 10.2458232 -05 21 55.292412   27.26651 21.7164 25.85518   ~ 3 0
26 AS2UDS J021810.98-044946.92 rG 02 18 10.9835038 -04 49 46.915258     23.6288 25.91556   ~ 5 0
27 AS2UDS 0121.1 G 02 18 11.00 -04 49 51.9     24.302 26.30396   ~ 4 0
28 AS2UDS 0291.0 G 02 18 21.4909445 -04 42 31.605295   25.91958 22.5193 24.53178   ~ 3 0
29 AS2UDS 0049.0 G 02 18 22.2485796 -05 29 50.469575   28.13641 22.6377 26.98543   ~ 3 0
30 AS2UDS 0712.0 G 02 18 23.0726150 -05 24 36.508524     23.4072 26.77917   ~ 3 0
31 AS2UDS 0268.0 G 02 18 33.7763662 -05 10 19.665299   26.81231 21.9014 25.55934   ~ 4 0
32 AS2UDS 0156.0 G 02 18 37.6167242 -05 16 15.381626   28.22013 22.2684 26.18121   ~ 3 0
33 AS2UDS 0026.0 G 02 19 02.05 -05 28 56.7   27.31057 23.7614 26.93315   ~ 8 0
34 AS2UDS 0223.0 G 02 19 03.0956767 -05 26 45.942767   27.04689 23.3486 25.85744   ~ 3 0
35 AS2UDS 0451.0 G 02 19 07.5977484 -05 00 18.934691   27.26177 23.3882 26.50724   ~ 3 0
36 AS2UDS 0209.0 G 02 19 07.9214618 -04 54 00.628761     23.1661 25.92077   ~ 3 0
37 AS2UDS 0039.0 G 02 19 09.74 -05 15 30.6   27.25570 23.1875 26.97022   ~ 5 0
38 AS2UDS 0082.0 G 02 19 12.7810562 -05 12 45.278492   27.17022 22.3887 26.18888   ~ 3 0
39 AS2UDS 0114.0 G 02 19 13.19 -04 47 08.0   25.47871 22.6341 24.49698   ~ 5 0
40 AS2UDS 0076.0 G 02 19 13.8210710 -05 19 48.051001   27.74044 22.9538 25.21365   ~ 3 0
41 AS2UDS 0461.0 G 02 19 25.4998138 -04 59 48.294789   27.86489 23.2033 26.55637   ~ 3 0

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