2024ApJ...969...54W


Query : 2024ApJ...969...54W

2024ApJ...969...54W - Astrophys. J., 969, 54 (2024/July-1)

Sp1149. I. Constraints on the Balmer L-σ Relation for H II Regions in a Spiral Galaxy at Redshift z = 1.49 Strongly Lensed by the MACS J1149 Cluster.

WILLIAMS H., KELLY P., CHEN W., DIEGO J.M., OGURI M. and FILIPPENKO A.V.

Abstract (from CDS):

The luminosities (L) and velocity dispersions (σ) of the extinction-corrected Balmer emission lines of giant H II regions in nearby galaxies exhibit a tight correlation (∼0.35 dex scatter). There are few constraints, however, on whether giant H II regions at significant look-back times follow an L-σ relation, given the angular resolution and sensitivity required to study them individually. We measure the luminosities and velocity dispersions of Hα and Hβ emission from 11 H II regions in Sp1149, a spiral galaxy at redshift (z) z = 1.49 multiply imaged by the MACS J1149 galaxy cluster. Sp1149 is also the host galaxy of the first-known strongly lensed supernova with resolved images, SN Refsdal. We employ archival Keck I OSIRIS observations, and newly acquired Keck I MOSFIRE and Large Binocular Telescope LUCI long-slit spectra of Sp1149. When we use the GLAFIC simply parameterized lens model, we find that the Hα luminosities of the H II regions at z = 1.49 are a factor of ${6.4}_{-2.0}^{+2.9}$ brighter than predicted by the low-redshift L-σ relation we measure from Very Large Telescope MUSE spectroscopy. If the lens model is accurate, then the H II regions in Sp1149 differ from their low-redshift counterparts. We identify an H II region in Sp1149 that is dramatically brighter (by 2.03 ± 0.44 dex) than our low-redshift L-σ relation predicts given its low velocity dispersion. Finally, the H II regions in Sp1149 are consistent, perhaps surprisingly, with the z ≈ 0 star-forming locus on the Baldwin-Phillips-Terlevich diagram.

Abstract Copyright: © 2024. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Gravitational lensing - Galactic and extragalactic astronomy - Galaxy clusters - H II regions - High-redshift galaxies

Simbad objects: 26

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Number of rows : 26
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 ASASSN -14hr SN* 01 50 41.230 -14 31 04.75           SNIa 11 0
2 LEDA 923603 G 01 50 41.2599709464 -14 31 03.138987072   15.59   14.75   ~ 12 0
3 ESO 153-20 Sy2 02 06 03.4672137720 -55 11 36.873277656   14.06 14.31 12.67 13.3 ~ 65 0
4 SN 2012U SN* 02 06 04.33 -55 11 37.5           SNIa 10 1
5 PSN J07250042+2347030 SN* 07 25 00.42 +23 47 03.0           SNIa 3 0
6 NGC 2370 GiG 07 25 01.6494155952 +23 46 59.402786196   14.3       ~ 33 0
7 ASASSN -15fr SN* 09 20 20.4 -07 38 27           SNIa-norm 12 0
8 LEDA 1015528 EmG 09 20 20.453 -07 38 22.96   15.93   15.20   ~ 9 0
9 LEDA 1264881 G 10 32 47.83921 +04 11 45.5567           ~ 8 0
10 LSQ 13ry SN* 10 32 48.00 +04 11 51.4           SNIa 16 0
11 MCG-04-27-009 G 11 23 41.3 -22 16 16           ~ 13 0
12 SN 2009aa SN* 11 23 42.28 -22 16 14.5           SNIa 33 1
13 HD 98989 * 11 23 46.4661158280 +34 14 33.808215984   9.25 9.24     A0V 29 0
14 HD 101060 Em* 11 37 57.8119863552 +15 46 36.854130612   8.77 8.78     A1V 38 0
15 CLASHVLT J114935.29+222345.6 LeG 11 49 35.278 +22 23 45.77         21.51 ~ 24 0
16 [KDR2018] LS1 LeI 11 49 35.66 +22 23 48.0           ~ 16 0
17 MCS J1149.5+2223 ClG 11 49 35.8 +22 23 55           ~ 546 0
18 NAME SN Refsdal SN* 11 49 36.010 +22 23 48.13           ~ 130 0
19 CLASHVLT J114936.81+222408.9 LeG 11 49 36.814 +22 24 08.88         22.63 ~ 16 0
20 HD 111744 * 12 51 23.3269209792 +12 22 21.999139572   8.86 8.86     A0V 36 0
21 Z 48-99 G 15 04 29.7329463456 +02 19 58.990425204   15.3       ~ 18 0
22 SN 2014ey SN* 15 04 29.970 +02 19 51.25           SNIax 6 0
23 ASASSN -14co SN* 15 57 29.910 +01 06 33.74           SNIa 7 0
24 Z 23-5 G 15 57 30.3 +01 06 40   15.5       ~ 14 0
25 SN 2013fy SN* 21 37 27.13 -47 01 55.6           SNIa 14 1
26 ESO 287-40 GiG 21 37 28.1844944568 -47 02 08.827431612   14.29   13.01   ~ 41 0

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