Effects of Halo Spin on the Formation and Evolution of Bars in Disk Galaxies
The spin of dark halos has been shown to significantly affect bar formation and evolution in disk galaxies. To understand the physical role of halo spin in bar formation, we run N -body simulations of isolated, Milky Way–sized galaxies by varying the halo spin parameter in the range −0.16 ≤ λ ≤ 0.16...
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Published in | The Astrophysical journal Vol. 971; no. 1; pp. 67 - 81 |
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Format | Journal Article |
Language | English |
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01.08.2024
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Abstract | The spin of dark halos has been shown to significantly affect bar formation and evolution in disk galaxies. To understand the physical role of halo spin in bar formation, we run
N
-body simulations of isolated, Milky Way–sized galaxies by varying the halo spin parameter in the range −0.16 ≤
λ
≤ 0.16 and the bulge mass. We find that our adopted halo
alone
is subject to swing amplification of an
m
= 2 nonaxisymmetric mode rotating in the same sense as the halo, which assists or inhibits the bar formation in a disk depending on its sense of rotation. The
m
= 2 mode in the disk, growing via swing amplification, interacts constructively (destructively) with the
m
= 2 mode in the prograde (retrograde) halo, promoting (delaying) bar formation. A bar grows by losing its angular momentum primarily to a halo. Since the halo particles inside (outside) the corotation resonance with the bar can emit (absorb) angular momentum to (from) the bar, the bar pattern speed decays more slowly for larger
λ
> 0, while it decreases relatively fast almost independent of
λ
≤ 0. Models with a strong bar develop a boxy peanut-shaped bulge. In models without a bulge, this occurs rapidly via buckling instability, while bars with a bulge thicken gradually without undergoing buckling instability. Among the models considered in the present work, the bar in the
λ
= 0.06 model with a bulge of 10% of the disk mass best describes the Milky Way in terms of its length and pattern speed. |
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AbstractList | The spin of dark halos has been shown to significantly affect bar formation and evolution in disk galaxies. To understand the physical role of halo spin in bar formation, we run N -body simulations of isolated, Milky Way–sized galaxies by varying the halo spin parameter in the range −0.16 ≤ λ ≤ 0.16 and the bulge mass. We find that our adopted halo alone is subject to swing amplification of an m = 2 nonaxisymmetric mode rotating in the same sense as the halo, which assists or inhibits the bar formation in a disk depending on its sense of rotation. The m = 2 mode in the disk, growing via swing amplification, interacts constructively (destructively) with the m = 2 mode in the prograde (retrograde) halo, promoting (delaying) bar formation. A bar grows by losing its angular momentum primarily to a halo. Since the halo particles inside (outside) the corotation resonance with the bar can emit (absorb) angular momentum to (from) the bar, the bar pattern speed decays more slowly for larger λ > 0, while it decreases relatively fast almost independent of λ ≤ 0. Models with a strong bar develop a boxy peanut-shaped bulge. In models without a bulge, this occurs rapidly via buckling instability, while bars with a bulge thicken gradually without undergoing buckling instability. Among the models considered in the present work, the bar in the λ = 0.06 model with a bulge of 10% of the disk mass best describes the Milky Way in terms of its length and pattern speed. The spin of dark halos has been shown to significantly affect bar formation and evolution in disk galaxies. To understand the physical role of halo spin in bar formation, we run N -body simulations of isolated, Milky Way–sized galaxies by varying the halo spin parameter in the range −0.16 ≤ λ ≤ 0.16 and the bulge mass. We find that our adopted halo alone is subject to swing amplification of an m = 2 nonaxisymmetric mode rotating in the same sense as the halo, which assists or inhibits the bar formation in a disk depending on its sense of rotation. The m = 2 mode in the disk, growing via swing amplification, interacts constructively (destructively) with the m = 2 mode in the prograde (retrograde) halo, promoting (delaying) bar formation. A bar grows by losing its angular momentum primarily to a halo. Since the halo particles inside (outside) the corotation resonance with the bar can emit (absorb) angular momentum to (from) the bar, the bar pattern speed decays more slowly for larger λ > 0, while it decreases relatively fast almost independent of λ ≤ 0. Models with a strong bar develop a boxy peanut-shaped bulge. In models without a bulge, this occurs rapidly via buckling instability, while bars with a bulge thicken gradually without undergoing buckling instability. Among the models considered in the present work, the bar in the λ = 0.06 model with a bulge of 10% of the disk mass best describes the Milky Way in terms of its length and pattern speed. |
Author | Jang, Dajeong Kim, Woong-Tae |
Author_xml | – sequence: 1 givenname: Dajeong orcidid: 0000-0002-7202-4373 surname: Jang fullname: Jang, Dajeong organization: Seoul National University Department of Physics & Astronomy, Seoul 08826, Republic of Korea – sequence: 2 givenname: Woong-Tae orcidid: 0000-0003-4625-229X surname: Kim fullname: Kim, Woong-Tae organization: Seoul National University SNU Astronomy Research Center, Seoul 08826, Republic of Korea |
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SubjectTerms | Amplification Angular momentum Barred spiral galaxies Buckling Corotation Disk galaxies Evolution Galactic evolution Galactic halos Galaxy bars Galaxy bulges Galaxy dark matter halos Galaxy disks Milky Way Milky Way Galaxy Particle decay Rotating bodies Rotating disks |
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Title | Effects of Halo Spin on the Formation and Evolution of Bars in Disk Galaxies |
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