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Published September 2009 | Published
Journal Article Open

Forming a large disc galaxy from a z < 1 major merger

Abstract

Using high-resolution SPH simulations in a fully cosmological Λ cold dark matter context, we study the formation of a bright disc-dominated galaxy that originates from a 'wet' major merger at z = 0.8 . The progenitors of the disc galaxy are themselves disc galaxies that formed from early major mergers between galaxies with blue colours. A substantial thin stellar disc grows rapidly following the last major merger and the present-day properties of the final remnant are typical of early-type spiral galaxies, with an i-band bulge-to-disc ratio ~0.65, a disc scalelength of 7.2 kpc, g−r = 0.5 mag , an HI linewidth (W_(20)/2) of 238 km s^(−1) and total magnitude i = −22.4. The key ingredients for the formation of a dominant stellar disc component after a major merger are (i) substantial and rapid accretion of gas through cold flows followed at late times by cooling of gas from the hot phase, (ii) supernova feedback that is able to partially suppress star formation during mergers and (iii) relative fading of the spheroidal component. The gas fraction of the progenitors' discs does not exceed 25 per cent at z < 3 , emphasizing that the continuous supply of gas from the local environment plays a major role in the regrowth of discs and in keeping the galaxies blue. The results of this simulation alleviate the problem posed for the existence of disc galaxies by the high likelihood of interactions and mergers for galaxy-sized haloes at relatively low z.

Additional Information

© 2009 RAS. Accepted 2009 May 24. Received 2009 April 27; in original form 2008 December 30. Simulations were run at ARSC, NASA AMES and Texas Supercomputing Center. FG acknowledges support from a Theodore Dunham grant, HST GO-1125, NSF ITR grant PHY-0205413 (also supporting TQ), NSF grant AST-0607819 and NASA ATP NNX08AG84G. CBB acknowledges the support of UK's Science & Technology Facilities Council (ST/F002432/1). PJ was supported by programmes HST-AR-10678 and 10958 and by Spitzer Theory Grant 30183 from the Jet Propulsion Laboratory.We acknowledge discussions with several smart people, among them Avishai Dekel, Mark Fardal, James Bullock and Phil Hopkins. FG and AMB acknowledge the hospitality of the Max Planck Institute during the writing of this paper.

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August 21, 2023
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