Constraints on the Assembly History of the Milky Way's Smooth, Diffuse Stellar Halo from the Metallicity-dependent, Radially Dominated Velocity Anisotropy Profiles Probed with K Giants and BHB Stars Using LAMOST, SDSS/SEGUE, and Gaia
We analyze the anisotropy profile of the Milky Way’s smooth, diffuse stellar halo using the Sloan Digital Sky Survey (SDSS) SEGUE blue horizontal branch stars and the SDSS/SEGUE and LAMOST K giants. These intrinsically luminous stars allow us to probe the halo to approximately 100 kpc from the Galac...
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Published in | The Astrophysical journal Vol. 919; no. 1; pp. 66 - 92 |
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Main Authors | , , , , , , , |
Format | Journal Article |
Language | English |
Published |
Philadelphia
The American Astronomical Society
01.09.2021
IOP Publishing |
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Abstract | We analyze the anisotropy profile of the Milky Way’s smooth, diffuse stellar halo using the Sloan Digital Sky Survey (SDSS) SEGUE blue horizontal branch stars and the SDSS/SEGUE and LAMOST K giants. These intrinsically luminous stars allow us to probe the halo to approximately 100 kpc from the Galactic center. Line-of-sight velocities, distances, metallicities, and proper motions are available for all stars via SDSS/SEGUE, LAMOST, and Gaia, and we use these data to construct a full 7D set consisting of positions, space motions, and metallicity. We remove substructure from our samples using integrals of motion based on the method of Xue et al. We find radially dominated kinematic profiles with nearly constant anisotropy within 20 kpc, beyond which the anisotropy profile gently declines but remains radially dominated to the farthest extents of our sample. Independent of star type or substructure removal, the anisotropy depends on metallicity, such that the orbits of the stars become less radial with decreasing metallicity. For −1.7 < [Fe/H] < −1, the smooth, diffuse halo anisotropy profile begins to decline at Galactocentric distances ∼20 kpc, from
β
∼
0.9
to 0.7 for K giants and from
β
∼
0.8
to 0.1 for blue horizontal branch stars. For [Fe/H] < −1.7, the smooth, diffuse halo anisotropy remains constant along all distances with
0.2
<
β
<
0.7
depending on the metallicity range probed, but independent of star type. These samples are ideal for estimating the total Galactic mass as they represent the virialized stellar halo system. |
---|---|
AbstractList | We analyze the anisotropy profile of the Milky Way’s smooth, diffuse stellar halo using the Sloan Digital Sky Survey (SDSS) SEGUE blue horizontal branch stars and the SDSS/SEGUE and LAMOST K giants. These intrinsically luminous stars allow us to probe the halo to approximately 100 kpc from the Galactic center. Line-of-sight velocities, distances, metallicities, and proper motions are available for all stars via SDSS/SEGUE, LAMOST, and Gaia, and we use these data to construct a full 7D set consisting of positions, space motions, and metallicity. We remove substructure from our samples using integrals of motion based on the method of Xue et al. We find radially dominated kinematic profiles with nearly constant anisotropy within 20 kpc, beyond which the anisotropy profile gently declines but remains radially dominated to the farthest extents of our sample. Independent of star type or substructure removal, the anisotropy depends on metallicity, such that the orbits of the stars become less radial with decreasing metallicity. For −1.7 < [Fe/H] < −1, the smooth, diffuse halo anisotropy profile begins to decline at Galactocentric distances ∼20 kpc, from \(\beta \sim 0.9\) to 0.7 for K giants and from \(\beta \sim 0.8\) to 0.1 for blue horizontal branch stars. For [Fe/H] < −1.7, the smooth, diffuse halo anisotropy remains constant along all distances with \(0.2\lt \beta \lt 0.7\) depending on the metallicity range probed, but independent of star type. These samples are ideal for estimating the total Galactic mass as they represent the virialized stellar halo system. We analyze the anisotropy profile of the Milky Way’s smooth, diffuse stellar halo using the Sloan Digital Sky Survey (SDSS) SEGUE blue horizontal branch stars and the SDSS/SEGUE and LAMOST K giants. These intrinsically luminous stars allow us to probe the halo to approximately 100 kpc from the Galactic center. Line-of-sight velocities, distances, metallicities, and proper motions are available for all stars via SDSS/SEGUE, LAMOST, and Gaia, and we use these data to construct a full 7D set consisting of positions, space motions, and metallicity. We remove substructure from our samples using integrals of motion based on the method of Xue et al. We find radially dominated kinematic profiles with nearly constant anisotropy within 20 kpc, beyond which the anisotropy profile gently declines but remains radially dominated to the farthest extents of our sample. Independent of star type or substructure removal, the anisotropy depends on metallicity, such that the orbits of the stars become less radial with decreasing metallicity. For −1.7 < [Fe/H] < −1, the smooth, diffuse halo anisotropy profile begins to decline at Galactocentric distances ∼20 kpc, from β ∼ 0.9 to 0.7 for K giants and from β ∼ 0.8 to 0.1 for blue horizontal branch stars. For [Fe/H] < −1.7, the smooth, diffuse halo anisotropy remains constant along all distances with 0.2 < β < 0.7 depending on the metallicity range probed, but independent of star type. These samples are ideal for estimating the total Galactic mass as they represent the virialized stellar halo system. |
Author | Liu, Chao Shen, Juntai Yang, Chengqun Bird, Sarah A. Flynn, Chris Zhao, Gang Tian, Hai-Jun Xue, Xiang-Xiang |
Author_xml | – sequence: 1 givenname: Sarah A. orcidid: 0000-0002-5469-5149 surname: Bird fullname: Bird, Sarah A. organization: Key Laboratory for Research in Galaxies and Cosmology, Shanghai Astronomical Observatory, 80 Nandan Road, Shanghai 200030, People's Republic of China – sequence: 2 givenname: Xiang-Xiang orcidid: 0000-0002-0642-5689 surname: Xue fullname: Xue, Xiang-Xiang organization: University of Chinese Academy of Sciences School of Astronomy and Space Science, Beijing 100049, People’s Republic of China – sequence: 3 givenname: Chao orcidid: 0000-0002-1802-6917 surname: Liu fullname: Liu, Chao organization: Chinese Academy of Sciences Key Laboratory of Space Astronomy and Technology, National Astronomical Observatories, Beijing 100101, People's Republic of China – sequence: 4 givenname: Juntai orcidid: 0000-0001-5604-1643 surname: Shen fullname: Shen, Juntai organization: Key Laboratory for Particle Astrophysics and Cosmology (MOE) / Shanghai Key Laboratory for Particle Physics and Cosmology, Shanghai 200240, People's Republic of China – sequence: 5 givenname: Chris orcidid: 0000-0002-4796-745X surname: Flynn fullname: Flynn, Chris organization: ARC Centre of Excellence for Gravitational Wave Discovery (OzGrav), Australia – sequence: 6 givenname: Chengqun orcidid: 0000-0003-1972-0086 surname: Yang fullname: Yang, Chengqun organization: Key Laboratory for Research in Galaxies and Cosmology, Shanghai Astronomical Observatory, 80 Nandan Road, Shanghai 200030, People's Republic of China – sequence: 7 givenname: Gang orcidid: 0000-0002-8980-945X surname: Zhao fullname: Zhao, Gang organization: University of Chinese Academy of Sciences School of Astronomy and Space Science, Beijing 100049, People’s Republic of China – sequence: 8 givenname: Hai-Jun orcidid: 0000-0001-9289-0589 surname: Tian fullname: Tian, Hai-Jun organization: China Three Gorges University Center for Astronomy and Space Sciences, Yichang 443002, People's Republic of China |
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CitedBy_id | crossref_primary_10_1016_j_xinn_2022_100224 crossref_primary_10_3847_1538_4357_acd33d crossref_primary_10_1093_mnras_stad2681 crossref_primary_10_3847_1538_4357_acd33a crossref_primary_10_1016_j_newar_2024_101706 crossref_primary_10_3847_1538_3881_ac746e crossref_primary_10_3847_2515_5172_ac6ef3 crossref_primary_10_1088_1538_3873_acea43 crossref_primary_10_1093_mnras_stac2036 crossref_primary_10_3847_1538_4357_ac31ac crossref_primary_10_1093_mnras_stac3581 crossref_primary_10_3847_1538_4357_ac8d68 crossref_primary_10_1093_mnras_stac2666 crossref_primary_10_3847_1538_4357_ac86c7 crossref_primary_10_3847_1538_3881_ac9900 crossref_primary_10_1088_1674_4527_ac9e91 crossref_primary_10_1093_mnras_stad3860 crossref_primary_10_1093_mnras_stad706 crossref_primary_10_3847_1538_4357_ad19ca crossref_primary_10_1093_mnras_stad2138 crossref_primary_10_3847_1538_4357_ace533 crossref_primary_10_3788_gzxb20235205_0552212 crossref_primary_10_3847_1538_3881_ad33bb crossref_primary_10_3847_1538_4357_ad31a6 crossref_primary_10_1093_mnras_stae1363 crossref_primary_10_1038_s41550_020_01254_3 crossref_primary_10_1051_0004_6361_202141570 |
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Copyright | 2021. The American Astronomical Society. All rights reserved. Copyright IOP Publishing Sep 01, 2021 |
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Snippet | We analyze the anisotropy profile of the Milky Way’s smooth, diffuse stellar halo using the Sloan Digital Sky Survey (SDSS) SEGUE blue horizontal branch stars... |
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SubjectTerms | Anisotropy Astrophysics Galactic mass Horizontal branch stars Metallicity Milky Way Milky Way stellar halo Sky surveys (astronomy) |
Title | Constraints on the Assembly History of the Milky Way's Smooth, Diffuse Stellar Halo from the Metallicity-dependent, Radially Dominated Velocity Anisotropy Profiles Probed with K Giants and BHB Stars Using LAMOST, SDSS/SEGUE, and Gaia |
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