Abstract

The structure of the Sun’s corona varies with the solar-cycle phase, from a near spherical symmetry at solar maximum to an axial dipole at solar minimum. It is widely accepted that the large-scale coronal structure is governed by magnetic fields that are most likely generated by dynamo action in the solar interior. In order to understand the variation in coronal structure, we couple a potential-field source-surface model with a cyclic dynamo model. In this coupled model, the magnetic field inside the convection zone is governed by the dynamo equation; these dynamo-generated fields are extended from the photosphere to the corona using a potential-field source-surface model. Assuming axisymmetry, we take linear combinations of associated Legendre polynomials that match the more complex coronal structures. Choosing images of the global corona from the Mauna Loa Solar Observatory at each Carrington rotation over half a cycle (1986 – 1991), we compute the coefficients of the associated Legendre polynomials up to degree eight and compare with observations. We show that at minimum the dipole term dominates, but it fades as the cycle progresses; higher-order multipolar terms begin to dominate. The amplitudes of these terms are not exactly the same for the two limbs, indicating that there is a longitude dependence. While both the 1986 and the 1996 minimum coronas were dipolar, the minimum in 2008 was unusual, since there was a substantial departure from a dipole. We investigate the physical cause of this departure by including a North–South asymmetry in the surface source of the magnetic fields in our flux-transport dynamo model, and find that this asymmetry could be one of the reasons for departure from the dipole in the 2008 minimum.

Highlights

  • The coronal structure seen in white-light coronagraphs and solar-eclipse images evolves through a sequence of patterns in which the relative strength of the axial dipole and higher multipoles varies with cycle phase

  • Our primary result is that low-order axisymmetric Legendre polynomials can be used to represent white-light coronal structures that are similar to the output of a flux-transport dynamo coupled with a potential-field source-surface model, as these structures evolve over a solar cycle, and differ for minima of different cycles

  • The main limitation of this approach is the absence of longitude dependence in the polynomials that could capture the presence of different coronal structures at the same time in the East and West limbs of the Sun

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Summary

Introduction

The coronal structure seen in white-light coronagraphs and solar-eclipse images evolves through a sequence of patterns in which the relative strength of the axial dipole and higher multipoles varies with cycle phase. Near the maximum in 1990, we can see that the corona, as revealed by the total solar eclipse on 22 July 1990, picture taken in Russia, looks almost spherically symmetric (panel a). By 1994 the cycle is in its descending phase (panel b) In this image, taken in Bolivia during the total solar eclipse on 3 November 1994, we start seeing the appearance of dipolar structure. In panel c, produced from the total solar-eclipse image during 24 October 1995, taken in India, the dipole structure is extremely clear. By 1998 (panel d), we are in the ascending phase of Cycle 23 and we can see, from the image during the total solar eclipse on 26 February 1998, Dynamo–PFSS Corona taken in Aruba, the evolution of the strong dipole structure into a smoother, more spherically symmetric pattern once more

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