2021A&A...653A.111R


Query : 2021A&A...653A.111R

2021A&A...653A.111R - Astronomy and Astrophysics, volume 653A111-111 (2021/9-1)

The ALPINE-ALMA [CII] survey. The contribution of major mergers to the galaxy mass assembly at z ∼ 5.

ROMANO M., CASSATA P., MORSELLI L., JONES G.C., GINOLFI M., ZANELLA A., BETHERMIN M., CAPAK P., FAISST A., LE FEVRE O., SCHAERER D., SILVERMAN J.D., YAN L., BARDELLI S., BOQUIEN M., CIMATTI A., DESSAUGES-ZAVADSKY M., ENIA A., FUJIMOTO S., GRUPPIONI C., HATHI N.P., IBAR E., KOEKEMOER A.M., LEMAUX B.C., RODIGHIERO G., VERGANI D., ZAMORANI G. and ZUCCA E.

Abstract (from CDS):


Context. Galaxy mergers are thought to be one of the main mechanisms of the mass assembly of galaxies in the Universe, but there is still little direct observational evidence of how frequent they are at z≤4. Recently, many works have suggested a possible increase in the fraction of major mergers in the early Universe, reviving the debate on which processes (e.g., cold accretion, star formation, mergers) most contribute to the mass build-up of galaxies through cosmic time.
Aims. To estimate the importance of major mergers in this context, we make use of the new data collected by the ALMA Large Program to INvestigate [CII] at Early times (ALPINE) survey, which attempted to observe the [CII] 158µm emission line from a sample of 75 main-sequence star-forming galaxies at 4.4<z<5.9.
Methods. We used, for the first time, the morpho-kinematic information provided by the [CII] emission, along with archival multiwavelength data to obtain the fraction of major mergers (fMM) at z∼5. By combining the results from ALPINE with those at lower redshifts from the literature, we also studied the evolution of the merger fraction through cosmic time. We then used different redshift-evolving merger timescales (TMM) to convert this fraction into the merger rate per galaxy (RMM) and in the volume-averaged merger rate (ΓMM).
Results. We find a merger fraction of fMM∼0.44(0.34) at z∼4.5(5.5) from ALPINE. By combining our results with those at lower redshifts, we computed the cosmic evolution of the merger fraction which is described by a rapid increase from the local Universe to higher redshifts, a peak at z∼3, and a slow decrease toward earlier epochs. Depending on the timescale prescription used, this fraction translates into a merger rate ranging between ∼0.1 and ∼4.0Gyr–1 at z∼5, which in turn corresponds to an average number of major mergers per galaxy between 1 and 8 in ∼12.5yr (from z=6 to the local Universe). When convolved with the galaxy number density at different epochs, the merger rate density becomes approximately constant over time at 1<z<4, including values from 10–4 to 10–3Gyr–1Mpc–3, depending on the assumed TMM. We finally compare the specific star formation and star-formation rate density with the analogous quantities from major mergers, finding a good agreement at z>4 if we assume a merger timescale that quickly decreases with increasing redshift.
Conclusions. Our new constraints on the merger fraction from the ALPINE survey at z∼5 reveal the presence of a significant merging activity in the early Universe. Whether this population of mergers can provide a relevant contribution to the galaxy mass assembly at these redshifts and through the cosmic epochs is strongly dependent on the assumption of the merger timescale. However, our results show that an evolving TMM∝(1+z)–2 agrees well with state-of-the-art cosmological simulations, suggesting a considerable role of mergers in the build-up of galaxies at early times.

Abstract Copyright: © ESO 2021

Journal keyword(s): galaxies: evolution - galaxies: formation - galaxies: high-redshift - galaxies: kinematics and dynamics - early Universe

Simbad objects: 28

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Number of rows : 28
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 GOODS J033215.90-274123.9 EmG 03 32 15.8971 -27 41 23.880   28.5930     26.6639 ~ 20 0
2 NAME Extended Chandra Deep Field South reg 03 32 30.0 -27 48 20           ~ 862 0
3 NAME Hubble Ultra Deep Field reg 03 32 39.0 -27 47 29           ~ 1900 0
4 COSMOS2015 665509 EmG 09 58 56.45 +02 18 39.3   28.091 26.109 25.08 24.31 ~ 11 0
5 COSMOS2015 514583 EmG 09 58 57.91 +02 04 51.5     27.565 25.90 24.59 ~ 27 0
6 COSMOS2015 519281 EmG 09 59 00.90 +02 05 27.6   27.66   27.85 25.55 ~ 20 0
7 COSMOS2015 834764 EmG 09 59 35.73 +02 34 00.6     26.015 24.83 24.01 ~ 12 0
8 COSMOS2015 372292 EmG 09 59 39.170 +01 51 28.30           ~ 11 0
9 COSMOS2015 536534 EmG 09 59 53.250 +02 07 05.60     27.16 27.87 25.65 ~ 45 0
10 COSMOS2015 859732 EmG 10 00 00.490 +02 36 19.30           ~ 12 0
11 COSMOS2015 873321 EmG 10 00 04.05 +02 37 35.9     27.494 26.12 24.35 ~ 50 0
12 COSMOS2015 493583 EmG 10 00 23.36 +02 03 04.4     26.434 25.32 24.57 ~ 16 0
13 NAME COSMOS Field reg 10 00 28.60 +02 12 21.0           ~ 3639 0
14 COSMOS2015 842313 EmG 10 00 54.52 +02 34 35.2   27.842       ~ 43 0
15 CRISTAL 06 EmG 10 01 00.930 +01 48 33.84           ~ 21 0
16 COSMOS2015 773957 EmG 10 01 10.060 +02 28 29.20           ~ 15 0
17 COSMOS2015 680104 EmG 10 01 10.14 +02 19 56.3   28.885 26.506     ~ 13 0
18 COSMOS2015 378903 EmG 10 01 11.41846 +01 52 06.2184           ~ 7 0
19 COSMOS2015 434239 EmG 10 01 17.12 +01 57 19.2     26.840 25.78 24.52 ~ 18 0
20 NAME Taralay Protocluster PCG 10 01 24.80 +02 20 16.6           ~ 26 0
21 COSMOS2015 308643 EmG 10 01 26.68 +01 45 26.3     26.049 24.80 23.93 ~ 16 0
22 COSMOS2015 814483 EmG 10 01 27.16 +02 32 10.2 27.31 26.889 25.955 25.06 24.04 ~ 12 0
23 COSMOS2015 705527 EmG 10 01 33.45 +02 22 10.3   27.359 26.007 25.34 24.08 ~ 15 0
24 COSMOS2015 551281 EmG 10 01 37.47 +02 08 23.6     26.59 25.29 24.68 ~ 17 0
25 COSMOS2015 818760 EmG 10 01 54.86 +02 32 31.5     27.205 26.26 24.27 ~ 31 0
26 COSMOS2015 422677 EmG 10 01 59.46 +01 56 13.1 27.57 27.679 26.788 25.45 24.69 ~ 19 0
27 COSMOS2015 417567 EmG 10 02 04.098 +01 55 44.05           ~ 39 0
28 NAME HDF-S reg 22 32 56 -60 33.0           ~ 580 0

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