A Comprehensive Study of Hα Emitters at z ∼ 0.62 in the DAWN Survey: The Need for Deep and Wide Regions
Abstract We present new estimates of the luminosity function (LF) and star formation rate density (SFRD) for an H α -selected sample at z ∼ 0.62 from the Deep And Wide Narrow-band (DAWN) survey. Our results are based on a new H α sample in the extended COSMOS region (compared to Coughlin et al.) wi...
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Published in: | The Astrophysical journal Vol. 892; no. 1; p. 30 |
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Main Authors: | , , , , , , , , , , , , , , , , , , , , , |
Format: | Journal Article |
Language: | English |
Published: |
Philadelphia
IOP Publishing
20-03-2020
American Astronomical Society |
Subjects: | |
Online Access: | Get full text |
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Summary: | Abstract
We present new estimates of the luminosity function (LF) and star formation rate density (SFRD) for an H
α
-selected sample at
z
∼ 0.62 from the Deep And Wide Narrow-band (DAWN) survey. Our results are based on a new H
α
sample in the extended COSMOS region (compared to Coughlin et al.) with the inclusion of flanking fields, resulting in a total area coverage of ∼1.5 deg
2
. A total of 241 H
α
emitters were selected based on robust selection criteria using spectrophotometric redshifts and broadband color–color classification. Given that dust extinction is a dominant uncertainty in the estimation of LF and SFRD, we explore the effect of different dust-correction prescriptions by calculating the LF and SFRD using a constant dust extinction correction, A
H
α
= 1 mag, a luminosity-dependent correction, and a stellar-mass-dependent correction. The resulting H
α
LFs are well fitted using Schechter functions with best-fit parameters:
L
* = 10
42.24
erg s
−1
,
ϕ
* = 10
−2.85
Mpc
−3
,
α
= −1.62 for constant dust correction,
L
erg s
−1
,
ϕ
* = 10
−2.8
Mpc
−3
,
α
= −1.39 for luminosity-dependent dust correction, and
L
* = 10
42.36
erg s
−1
,
ϕ
* = 10
−2.91
Mpc
−3
,
α
= −1.48, for stellar-mass-dependent dust correction. The deep and wide nature of the DAWN survey effectively samples H
α
emitters over a wide range of luminosities, thereby providing better constraints on both the faint and bright ends of the LF. Also, the SFRD estimates
ρ
SFR
= 10
−1.39
M
⊙
yr
−1
Mpc
−3
(constant dust correction),
ρ
SFR
= 10
−1.47
M
⊙
yr
−1
Mpc
−3
(luminosity-dependent dust correction), and
ρ
SFR
= 10
−1.46
M
⊙
yr
−1
Mpc
−3
(stellar-mass-dependent dust correction) are in good agreement with the evolution of SFRD across redshifts (0 <
z
< 2) seen from previous H
α
surveys. |
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ISSN: | 0004-637X 1538-4357 |
DOI: | 10.3847/1538-4357/ab7015 |