Abstract:Context. The origin of large-scale magnetic fields in spiral galaxies is still a theoretical riddle and better observational constraints are required to make further progress. Aims. In order to better determine the large-scale 3D-structure of magnetic fields in spiral galaxies we present a Faraday rotation analysis of the edge-on spiral galaxy NGC 5775. Methods. Deep radio-continuum observations in total power and linear polarization were performed at 8.46 GHz with the VLA and the 100-m Effelsberg telescope. T… Show more
“…This is expected as Faraday depolarization effects are usually strongest in this area because the thermal electron density, the LOS, and the magnetic field strength are largest. A depolarization along the midplane has already been observed in several other spiral edge-on galaxies, for example NGC 5775 (Soida et al 2011). Furthermore, if there is a magnetic field parallel to the disk accompanied by strong vertical magnetic fields above and below the disk, we also expect strong beam polarization along the region of the projected transition between both magnetic field components.…”
Section: Vertical Scale Heights Of the Total Intensity Emissionmentioning
confidence: 56%
“…The total magnetic field strength in the disk of NGC 4631, B t ≈ 9 ± 2 μG, is comparable to the total field strength of the star forming edge-on galaxy NGC 5775 (Soida et al 2011), but it is not as strong as the strength in the starburst galaxy NGC 253 (Heesen et al 2009) which also has strong star formation along its disk. However, the average strength of the total magnetic field in the halo, B t ≈ 10 ± 2 μG, is higher than in other the edgeon galaxies studied so far.…”
Section: Discussionmentioning
confidence: 87%
“…In the halo it is characterized by an overall X-shaped configuration and a strong perpendicular field above the galactic center. The edge-on spiral galaxies NGC 5775 (Soida et al 2011) andNGC 4666 (Soida 2005) also have strong perpendicular components above and below their galactic centers. Dynamo simulations by Hanasz et al (2009) may be able to explain not only this X-shaped morphology but also these vertical fields.…”
Section: Discussionmentioning
confidence: 99%
“…Where spiral arms are visible, the fields tend to be more ordered in the interarm regions. In all of the edge-on spiral galaxies studied up to now, the large-scale ordered fields in the disk lie plane-parallel along the disk of the galaxy and in the halo they have an X-shaped morphology (Krause 2009), sometimes with nearly vertical field components above and below the central region (e.g., in NGC 5775, Soida et al 2011). The disk-parallel A&A 560, A42 (2013) magnetic field is the expected edge-on projection of the spiral magnetic disk field seen in face-on galaxies.…”
Context. All of the edge-on spiral galaxies observed so far present a similar magnetic field configuration, which consists of a planeparallel field in the disk and an X-shaped field at larger z-distances from the plane of the galaxy. Only NGC 4631 seems to have a different field orientation in its disk. Along the eastern and western halves of the disk of NGC 4631 the magnetic field orientation is parallel to the galactic plane, but in the central region of the disk a vertical field seems to dominate. Aims. In order to clarify whether NGC 4631 has a unique magnetic field configuration in the central region along its disk, we present high-resolution Faraday-corrected polarization data. Methods. Radio continuum observations of NGC 4631 at 4.85 GHz were performed with the VLA. In addition, observations were made with the Effelsberg telescope at 4.85 GHz and at 8.35 GHz. These were analyzed together with archival VLA-data at 8.35 GHz. The single-dish and interferometer data were combined to recover the missing zero-spacings. Results. We determined an integrated total spectral index of α tot = −0.78 ± 0.04 and a nonthermal integrated spectral index of α nth = −0.87 ± 0.03. The vertical scale heights in NGC 4631 vary significantly in different regions within the galaxy and their mean values at 4.85 GHz are with 2.3 kpc (370 pc) for the thick (thin) disk higher than the mean values found so far in six other edge-on spiral galaxies. This may originate in the tidal interaction of NGC 4631 with its neighbouring galaxies. The rotation measures are characterized by a smooth large-scale distribution. Along the galactic plane the degree of Faraday depolarization is significantly high. We estimated a total magnetic field strength in the disk of NGC 4631 of B t ≈ 9 ± 2 μG and an ordered field strength of B ord ≈ 2 ± 1 μG. The total field strengths in the halo are of the order of the total magnetic field strength in the disk, whereas the ordered field strengths in the halo seem to be higher than the value in the disk. Conclusions. The derived distribution of rotation measures implies that NGC 4631 has a large-scale regular magnetic field configuration. Despite the strong Faraday depolarization along the galactic plane and the strong beam depolarization in the transition zone between the disk and halo, our research strongly indicates that the magnetic field orientation along the central 5-7 kpc of the disk is also plane-parallel. Therefore, we claim that NGC 4631 also has a magnetic field structure plane-parallel along its entire disk, similar to all other edge-on galaxies observed up to now.
“…This is expected as Faraday depolarization effects are usually strongest in this area because the thermal electron density, the LOS, and the magnetic field strength are largest. A depolarization along the midplane has already been observed in several other spiral edge-on galaxies, for example NGC 5775 (Soida et al 2011). Furthermore, if there is a magnetic field parallel to the disk accompanied by strong vertical magnetic fields above and below the disk, we also expect strong beam polarization along the region of the projected transition between both magnetic field components.…”
Section: Vertical Scale Heights Of the Total Intensity Emissionmentioning
confidence: 56%
“…The total magnetic field strength in the disk of NGC 4631, B t ≈ 9 ± 2 μG, is comparable to the total field strength of the star forming edge-on galaxy NGC 5775 (Soida et al 2011), but it is not as strong as the strength in the starburst galaxy NGC 253 (Heesen et al 2009) which also has strong star formation along its disk. However, the average strength of the total magnetic field in the halo, B t ≈ 10 ± 2 μG, is higher than in other the edgeon galaxies studied so far.…”
Section: Discussionmentioning
confidence: 87%
“…In the halo it is characterized by an overall X-shaped configuration and a strong perpendicular field above the galactic center. The edge-on spiral galaxies NGC 5775 (Soida et al 2011) andNGC 4666 (Soida 2005) also have strong perpendicular components above and below their galactic centers. Dynamo simulations by Hanasz et al (2009) may be able to explain not only this X-shaped morphology but also these vertical fields.…”
Section: Discussionmentioning
confidence: 99%
“…Where spiral arms are visible, the fields tend to be more ordered in the interarm regions. In all of the edge-on spiral galaxies studied up to now, the large-scale ordered fields in the disk lie plane-parallel along the disk of the galaxy and in the halo they have an X-shaped morphology (Krause 2009), sometimes with nearly vertical field components above and below the central region (e.g., in NGC 5775, Soida et al 2011). The disk-parallel A&A 560, A42 (2013) magnetic field is the expected edge-on projection of the spiral magnetic disk field seen in face-on galaxies.…”
Context. All of the edge-on spiral galaxies observed so far present a similar magnetic field configuration, which consists of a planeparallel field in the disk and an X-shaped field at larger z-distances from the plane of the galaxy. Only NGC 4631 seems to have a different field orientation in its disk. Along the eastern and western halves of the disk of NGC 4631 the magnetic field orientation is parallel to the galactic plane, but in the central region of the disk a vertical field seems to dominate. Aims. In order to clarify whether NGC 4631 has a unique magnetic field configuration in the central region along its disk, we present high-resolution Faraday-corrected polarization data. Methods. Radio continuum observations of NGC 4631 at 4.85 GHz were performed with the VLA. In addition, observations were made with the Effelsberg telescope at 4.85 GHz and at 8.35 GHz. These were analyzed together with archival VLA-data at 8.35 GHz. The single-dish and interferometer data were combined to recover the missing zero-spacings. Results. We determined an integrated total spectral index of α tot = −0.78 ± 0.04 and a nonthermal integrated spectral index of α nth = −0.87 ± 0.03. The vertical scale heights in NGC 4631 vary significantly in different regions within the galaxy and their mean values at 4.85 GHz are with 2.3 kpc (370 pc) for the thick (thin) disk higher than the mean values found so far in six other edge-on spiral galaxies. This may originate in the tidal interaction of NGC 4631 with its neighbouring galaxies. The rotation measures are characterized by a smooth large-scale distribution. Along the galactic plane the degree of Faraday depolarization is significantly high. We estimated a total magnetic field strength in the disk of NGC 4631 of B t ≈ 9 ± 2 μG and an ordered field strength of B ord ≈ 2 ± 1 μG. The total field strengths in the halo are of the order of the total magnetic field strength in the disk, whereas the ordered field strengths in the halo seem to be higher than the value in the disk. Conclusions. The derived distribution of rotation measures implies that NGC 4631 has a large-scale regular magnetic field configuration. Despite the strong Faraday depolarization along the galactic plane and the strong beam depolarization in the transition zone between the disk and halo, our research strongly indicates that the magnetic field orientation along the central 5-7 kpc of the disk is also plane-parallel. Therefore, we claim that NGC 4631 also has a magnetic field structure plane-parallel along its entire disk, similar to all other edge-on galaxies observed up to now.
“…In the past few years, high-sensitivity polarization observations have also revealed the presence in galactic halos of magnetic fields forming a general X pattern. These so-called X-shape magnetic fields are characterized by a vertical (i.e., perpendicular to the disk plane) component that increases with both galactic radius and height in the four quadrants (Tüllmann et al 2000;Soida 2005; Krause et al 2006;Krause 2009;Heesen et al 2009;Braun et al 2010;Soida et al 2011;Haverkorn & Heesen 2012).…”
Context. External spiral galaxies seen edge-on exhibit X-shape magnetic fields in their halos. Whether the halo of our own Galaxy also hosts an X-shape magnetic field is still an open question. Aims. We would like to provide the necessary analytical tools to test the hypothesis of an X-shape magnetic field in the Galactic halo. Methods. We propose a general method to derive analytical models of divergence-free magnetic fields whose field lines are assigned a specific shape. We then utilize our method to obtain four particular models of X-shape magnetic fields in galactic halos. In passing, we also derive two particular models of predominantly horizontal magnetic fields in galactic disks. All our field models have spiraling field lines with spatially varying pitch angle. Results. Our four halo field models do indeed lead to X patterns in synthetic synchrotron polarization maps. Their precise topologies can all be explained by the action of a wind blowing outward from the galactic disk or from the galactic center. In practice, our field models may be used for fitting purposes or as inputs to various theoretical problems.
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