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- Publisher Website: 10.1051/0004-6361/201322623
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Article: Constraints on the Galactic bar from the Hercules stream as traced with RAVE across the Galaxy â&dagger
Title | Constraints on the Galactic bar from the Hercules stream as traced with RAVE across the Galaxy â&dagger |
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Authors | Antoja, TeresaHelmi, AminaDehnen, WalterBienaymé, OlivierBland-Hawthorn, Joss BlandFamaey, BenoîtFreeman, Kenneth C.Gibson, Brad K.Gilmore, Gerard F.Grebel, Eva K.Kordopatis, GeorgesKunder, Andrea M.Minchev, IvanMunari, UlisseNavarro, Julio F.Parker, Quentin A.Reid, Warren A.Seabroke, George M.Siebert, ArnaudSteinmetz, MatthiasWatson, Fred G.Wyse, Rosemary F GZwitter, Tomaž |
Keywords | Galaxy: structure Galaxy: disk Galaxy: evolution Galaxy: kinematics and dynamics |
Issue Date | 2014 |
Citation | Astronomy and Astrophysics, 2014, v. 563 How to Cite? |
Abstract | Non-axisymmetries in the Galactic potential (spiral arms and bar) induce kinematic groups such as the Hercules stream. Assuming that Hercules is caused by the effects of the outer Lindblad resonance of the Galactic bar, we model analytically its properties as a function of position in the Galaxy and its dependence on the bar's pattern speed and orientation. Using data from the RAVE survey we find that the azimuthal velocity of the Hercules structure decreases as a function of Galactocentric radius, in a manner consistent with our analytical model. This allows us to obtain new estimates of the parameters of the Milky Way's bar. The combined likelihood function of the bar's pattern speed and angle has its maximum for a pattern speed of Ωb = (1.89 ± 0.08) × Ω0, where Ω0 is the local circular frequency. Assuming a solar radius of 8.05 kpc and a local circular velocity of 238 km s-1, this corresponds to Ωb = 56 ± 2 km s-1 kpc-1. On the other hand, the bar's orientation φb cannot be constrained with the available data. In fact, the likelihood function shows that a tight correlation exists between the pattern speed and the orientation, implying that a better description of our best fit results is given by the linear relation Ωb/Ω0 = 1.91 + 0.0044(φb(deg)- 48), with standard deviation of 0.02. For example, for an angle of φb = 30 deg the pattern speed is 54.0 ± 0.5 km s -1 kpc-1. These results are not very sensitive to the other Galactic parameters such as the circular velocity curve or the peculiar motion of the Sun, and are robust to biases in distance. © 2014 ESO. |
Persistent Identifier | http://hdl.handle.net/10722/209025 |
ISSN | 2023 Impact Factor: 5.4 2023 SCImago Journal Rankings: 1.896 |
ISI Accession Number ID |
DC Field | Value | Language |
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dc.contributor.author | Antoja, Teresa | - |
dc.contributor.author | Helmi, Amina | - |
dc.contributor.author | Dehnen, Walter | - |
dc.contributor.author | Bienaymé, Olivier | - |
dc.contributor.author | Bland-Hawthorn, Joss Bland | - |
dc.contributor.author | Famaey, Benoît | - |
dc.contributor.author | Freeman, Kenneth C. | - |
dc.contributor.author | Gibson, Brad K. | - |
dc.contributor.author | Gilmore, Gerard F. | - |
dc.contributor.author | Grebel, Eva K. | - |
dc.contributor.author | Kordopatis, Georges | - |
dc.contributor.author | Kunder, Andrea M. | - |
dc.contributor.author | Minchev, Ivan | - |
dc.contributor.author | Munari, Ulisse | - |
dc.contributor.author | Navarro, Julio F. | - |
dc.contributor.author | Parker, Quentin A. | - |
dc.contributor.author | Reid, Warren A. | - |
dc.contributor.author | Seabroke, George M. | - |
dc.contributor.author | Siebert, Arnaud | - |
dc.contributor.author | Steinmetz, Matthias | - |
dc.contributor.author | Watson, Fred G. | - |
dc.contributor.author | Wyse, Rosemary F G | - |
dc.contributor.author | Zwitter, Tomaž | - |
dc.date.accessioned | 2015-03-23T02:31:12Z | - |
dc.date.available | 2015-03-23T02:31:12Z | - |
dc.date.issued | 2014 | - |
dc.identifier.citation | Astronomy and Astrophysics, 2014, v. 563 | - |
dc.identifier.issn | 0004-6361 | - |
dc.identifier.uri | http://hdl.handle.net/10722/209025 | - |
dc.description.abstract | Non-axisymmetries in the Galactic potential (spiral arms and bar) induce kinematic groups such as the Hercules stream. Assuming that Hercules is caused by the effects of the outer Lindblad resonance of the Galactic bar, we model analytically its properties as a function of position in the Galaxy and its dependence on the bar's pattern speed and orientation. Using data from the RAVE survey we find that the azimuthal velocity of the Hercules structure decreases as a function of Galactocentric radius, in a manner consistent with our analytical model. This allows us to obtain new estimates of the parameters of the Milky Way's bar. The combined likelihood function of the bar's pattern speed and angle has its maximum for a pattern speed of Ωb = (1.89 ± 0.08) × Ω0, where Ω0 is the local circular frequency. Assuming a solar radius of 8.05 kpc and a local circular velocity of 238 km s-1, this corresponds to Ωb = 56 ± 2 km s-1 kpc-1. On the other hand, the bar's orientation φb cannot be constrained with the available data. In fact, the likelihood function shows that a tight correlation exists between the pattern speed and the orientation, implying that a better description of our best fit results is given by the linear relation Ωb/Ω0 = 1.91 + 0.0044(φb(deg)- 48), with standard deviation of 0.02. For example, for an angle of φb = 30 deg the pattern speed is 54.0 ± 0.5 km s -1 kpc-1. These results are not very sensitive to the other Galactic parameters such as the circular velocity curve or the peculiar motion of the Sun, and are robust to biases in distance. © 2014 ESO. | - |
dc.language | eng | - |
dc.relation.ispartof | Astronomy and Astrophysics | - |
dc.subject | Galaxy: structure | - |
dc.subject | Galaxy: disk | - |
dc.subject | Galaxy: evolution | - |
dc.subject | Galaxy: kinematics and dynamics | - |
dc.title | Constraints on the Galactic bar from the Hercules stream as traced with RAVE across the Galaxy â&dagger | - |
dc.type | Article | - |
dc.description.nature | link_to_subscribed_fulltext | - |
dc.identifier.doi | 10.1051/0004-6361/201322623 | - |
dc.identifier.scopus | eid_2-s2.0-84896796123 | - |
dc.identifier.volume | 563 | - |
dc.identifier.eissn | 1432-0746 | - |
dc.identifier.isi | WOS:000333798000060 | - |
dc.identifier.issnl | 0004-6361 | - |