In astrophysics, Zeeman–Doppler imaging is a tomographic technique dedicated to the cartography of stellar magnetic fields, as well as surface brightness or spots and temperature distributions.
This method makes use of the ability of magnetic fields to polarize the light emitted (or absorbed) in spectral lines formed in the stellar atmosphere (the Zeeman effect). The periodic modulation of Zeeman signatures during the stellar rotation is employed to make an iterative reconstruction of the vectorial magnetic field at stellar surface.
The method was first proposed by Marsh and Horne in 1988, as a way to interpret the emission line variations of cataclysmic variable stars.[1] This techniques is based on the principle of maximum entropy image reconstruction; it yields the simplest magnetic field geometry (as a spherical harmonics expansion) among the various solutions compatible with the data.[2]
This technique is the first to enable the reconstruction of the vectorial magnetic geometry of stars similar to the Sun. It is now offering the opportunity to undertake systematic studies of stellar magnetism and is also yielding information on the geometry of large arches that magnetic fields are able to develop above stellar surfaces. To collect the observations related to Zeeman-Doppler Imaging, astronomers use stellar spectropolarimeters like ESPaDOnS [3] at CFHT on Mauna Kea (Hawaii), HARPSpol [4] at the ESO's 3.6m telescope (La Silla Observatory, Chile), as well as NARVAL[5] at Bernard Lyot Telescope (Pic du Midi de Bigorre, France).
The technique is very reliable, as the reconstruction of the magnetic field maps with different algorithms yield almost identical results, even with poorly sampled data sets.[6] It makes use of high-resolution time-series spectropolarimetric observations (Stokes parameter spectra).[7] It has however been shown, from both numerical simulations[8] and observations,[9] that the magnetic field strength and complexity is underestimated if no linear polarization spectra is available from observations. Since linear polarization signatures are weaker compared circular polarization their detections are not as reliable, particularly for cool stars. Therefore, the observations are normally limited to only Stokes IV parameters.[10] With more modern spectropolarimeters such as the recently installed SPIRou[11] at CFHT and CRIRES+[12] at the Very Large Telescope (Chile) the sensitivity to linear polarization will increase, allowing for more detailed studies of cool stars in the future.
References
edit- ^ Marsh, T. R.; Horne, K. (1 November 1988). "Images of accretion discs – II. Doppler tomography". Monthly Notices of the Royal Astronomical Society. 235 (1): 269–286. Bibcode:1988MNRAS.235..269M. doi:10.1093/mnras/235.1.269.
- ^ Donati, J.-F.; Howarth, I. D.; Jardine, M. M.; Petit, P.; et al. (2006). "The surprising magnetic topology of τ Sco: fossil remnant or dynamo output?". Monthly Notices of the Royal Astronomical Society. 370 (2): 629–644. arXiv:astro-ph/0606156. Bibcode:2006MNRAS.370..629D. doi:10.1111/j.1365-2966.2006.10558.x. S2CID 7054292.
- ^ "ESPaDOnS". Archived from the original on 2020-02-21. Retrieved 2021-10-28.
- ^ "Archived copy". Archived from the original on 2016-03-05. Retrieved 2015-09-08.
{{cite web}}: CS1 maint: archived copy as title (link) - ^ "Home Page of Narval". www.ast.obs-mip.fr. Archived from the original on 2020-07-30. Retrieved 2021-10-28.
- ^ Hussain, G. A. J.; Donati, J.- F.; Collier Cameron, A.; Barnes, J. R. (11 November 2000). "Comparisons of images derived from independent Zeeman Doppler imaging codes". Monthly Notices of the Royal Astronomical Society. 318 (4): 961–973. Bibcode:2000MNRAS.318..961H. doi:10.1046/j.1365-8711.2000.03573.x.
- ^ Hackman, T.; Lehtinen, J.; Rosén, L.; Kochukhov, O.; Käpylä, M. J. (2016-03-01). "Zeeman-Doppler imaging of active young solar-type stars". Astronomy & Astrophysics. 587: A28. arXiv:1509.02285. doi:10.1051/0004-6361/201527320. ISSN 0004-6361.
- ^ Kochukhov, O.; Piskunov, N. (June 2002). "Doppler Imaging of stellar magnetic fields: II. Numerical experiments". Astronomy & Astrophysics. 388 (3): 868–888. Bibcode:2002A&A...388..868K. doi:10.1051/0004-6361:20020300. ISSN 0004-6361.
- ^ Rosén, L.; Kochukhov, O.; Wade, G. A. (2015-05-29). "First Zeeman Doppler Imaging of a Cool Star Using All Four Stokes Parameters". The Astrophysical Journal. 805 (2): 169. arXiv:1504.00176. Bibcode:2015ApJ...805..169R. doi:10.1088/0004-637X/805/2/169. ISSN 1538-4357. S2CID 118833875. Archived from the original on 2020-10-19. Retrieved 2020-10-12.
- ^ Hackman, T.; Kochukhov, O.; Viviani, M.; Warnecke, J.; Korpi-Lagg, M. J.; Lehtinen, J. J. (2024-02-01). "From convective stellar dynamo simulations to Zeeman-Doppler images". Astronomy & Astrophysics. 682: A156. arXiv:2306.07838. doi:10.1051/0004-6361/202347144. ISSN 0004-6361.
- ^ "SPIRou". Archived from the original on 2020-02-21.
- ^ "ESO - CRIRES+". www.eso.org. Retrieved 2024-10-02.