2014
DOI: 10.1007/978-3-662-44625-6_17
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Magnetic Fields in the Milky Way

Abstract: This chapter presents a review of observational studies to determine the magnetic field in the Milky Way, both in the disk and in the halo, focused on recent developments and on magnetic fields in the diffuse interstellar medium. I discuss some terminology which is confusingly or inconsistently used and try to summarize current status of our knowledge on magnetic field configurations and strengths in the Milky Way. Although many open questions still exist, more and more conclusions can be drawn on the large-sc… Show more

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Cited by 126 publications
(100 citation statements)
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“…By not correcting for the foreground RM, which is perhaps as high as 1500 rad m −2 , we overestimate | B | by 15%. For PSR J1746-2856 B = 33 µG, and for PSR J1746-2849 B = 16 µG, which are both much higher than the strength of the ordered and turbulent magnetic field in the vicinity of the Sun (1.5-2 µG and 3-6 µG, respectively: e.g., Haverkorn 2015). Strong magnetic fields are not uncommon in the GC: in their analysis of the 'Snake' NTF, Gray et al (1995) derived B ≈ 7 µG for the foreground ISM.…”
Section: Discussionmentioning
confidence: 95%
See 1 more Smart Citation
“…By not correcting for the foreground RM, which is perhaps as high as 1500 rad m −2 , we overestimate | B | by 15%. For PSR J1746-2856 B = 33 µG, and for PSR J1746-2849 B = 16 µG, which are both much higher than the strength of the ordered and turbulent magnetic field in the vicinity of the Sun (1.5-2 µG and 3-6 µG, respectively: e.g., Haverkorn 2015). Strong magnetic fields are not uncommon in the GC: in their analysis of the 'Snake' NTF, Gray et al (1995) derived B ≈ 7 µG for the foreground ISM.…”
Section: Discussionmentioning
confidence: 95%
“…However, the signs of the RMs of PSRs J1746-2856 and J1746-2849 contradict this particular solution. By combining the observed DMs and RMs, and correcting for the foreground contribution to DM, we derive LOS lengths of the magnetic field vector between ∼ 16 − 33 µG, which is much larger than the strength of the large-scale and small-scale magnetic field in the vicinity of the Sun (Haverkorn 2015). If the GC, including the warm ionized medium that is probed by our observations, is pervaded by a strong magnetic field, B ∼ 160 µG (Crocker et al 2011), then our measurements imply that the magnetic field makes an angle 12…”
Section: Discussionmentioning
confidence: 99%
“…The synchrotron polarization together with Faraday rotation can be used to explore the properties of magnetic field, which is termed the traditional Faraday rotation synthesis (e.g., Burn 1966;Brentjens & de Bruyn 2005;Frick et al 2011;Beck et al 2012). This technique recently applying to polarized observational data provides a significant insight into magnetic field structures of galaxies (e.g., Fletcher et al 2011;Beck & Wielebinski 2013;Haverkorn 2015 for a review) and the properties of the interstellar medium (ISM, e.g., Jelić et al 2015;Van Eck et al 2017;Dickey et al 2018).…”
Section: Introductionmentioning
confidence: 99%
“…Magnetic fields in the Milky Way's disk were recently reviewed [97][98][99][100][101]. Basically, there are large radial regions where the magnetic field direction is going clockwise (between 2 and 5 kpc from the Galactic Center; and between 7 and 12 kpc from the Galactic Center), or counterclockwise (between 5 and 7 kpc from the Galactic Center) -see [9].…”
Section: Magnetic Field Map and Relations To The Armsmentioning
confidence: 99%