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Helioseismology is the study of the propagation of wave oscillations, particularly acoustic pressure waves, in the Sun. Unlike seismic waves on Earth, solar waves have practically no shear component (s-waves). Solar pressure waves are believed to be generated by the turbulence in the convection zone near the surface of the sun.^{[1]} Certain frequencies are amplified by constructive interference. In other words, the turbulence "rings" the sun like a bell. The acoustic waves are transmitted to the outer photosphere of the sun, which is where the light generated through absorption of radiant energy from nuclear fusion at the centre of the sun, leaves the surface. These oscillations are detectable on almost any time series of solar images, but are best observed by measuring the Doppler shift of photospheric absorption lines. Changes in the propagation of oscillation waves through the Sun reveal inner structures and allow astrophysicists to develop extremely detailed profiles of the interior conditions of the Sun.
Helioseismology was able to rule out the possibility that the solar neutrino problem was due to incorrect models of the interior of the Sun.^{[2]} Features revealed by helioseismology include that the outer convective zone and the inner radiative zone rotate at different speeds, which is thought to generate the main magnetic field of the Sun by a dynamo effect,^{[3]}^{[4]} and that the convective zone has "jet streams" of plasma (more precisely, torsional oscillations) thousands of kilometers below the surface.^{[5]} These jet streams form broad fronts at the equator, breaking into smaller cyclonic storms at high latitudes. Torsional oscillations are the time variation in solar differential rotation. They are alternating bands of faster and slower rotation. So far there is no generally accepted theoretical explanation for them, even though a close relation to the solar cycle is evident, as they have a period of eleven years, as was known since they were first observed in 1980.^{[6]}
Helioseismology can also be used to image the far side of the Sun from the Earth,^{[7]} including sunspots. In simple terms, sunspots absorb helioseismic waves. This sunspot absorption causes a seismic deficit that can be imaged at the antipode of the sunspot.^{[8]} To facilitate spaceweather forecasting, seismic images of the central portion of the solar far side have been produced nearly continuously since late 2000 by analysing data from the SOHO spacecraft, and since 2001 the entire far side has been imaged with this data.
Despite the name, helioseismology is the study of solar waves and not solar seismic activity. The name is derived from the similar practice of studying terrestrial seismic waves to determine the composition of the Earth's interior. The science can be compared to asteroseismology, which studies the propagation of sound waves in stars.
Individual oscillations in the Sun are damped so that they die out within a few periods. However, interference between these localised waves produces global standing waves, also known as normal modes. Analysis of these overlapping modes constitutes the discipline of global helioseismology.
Solar oscillation modes are essentially divided up into three categories, based on the restoring force that drives them: acoustic, gravity, and surface-gravity wave modes.
The data from time-series of solar spectra show all the oscillations overlapping. Thousands of modes have been detected (with the true number perhaps being in the millions). The mathematical technique of Fourier analysis is used to recover information about individual modes from this mass of data. The idea is that any periodic function f can be written as a sum of multiples of the simplest periodic functions, which are sines and cosines (of different frequencies). To find out how much (the amplitude) of each simple function goes into f, one applies the Fourier transform: at each point the value of this transform is obtained by computing a particular integral involving a modified version of f.
The simplest modes to analyse are the radial ones; however most solar modes are non-radial. A nonradial mode is characterized by three wavenumbers: the spherical-harmonic degree l and azimuthal order m which determine the behaviour of the mode over the surface of the star and the radial order n which reflects the properties in the radial direction (see the diagram on the top right for an example). Note that if the Sun were spherically symmetric, the azimuthal order would exhibit degeneracy; however the rotation of the Sun (along with other perturbations), which leads to an equatorial bulge, lifts this degeneracy. By convention, n corresponds to the number of nodes of the radial eigenfunction, l indicates the total number of nodal lines on spheres, and m tells how many of these nodal lines cross the equator.
In general the frequencies \omega_{nlm} of stellar oscillations depend on all three wave numbers. It is convenient, however, to separate the frequency into the multiplet frequency \omega_{nl}, obtained as a suitable average over azimuthal order m and corresponding to the spherically symmetric structure of the star, and the frequency splitting \delta\omega_{nlm} = \omega_{nlm} - \omega_{nl}.
Analyses of oscillation data must attempt to separate these different frequency components. In the case of the Sun the oscillations can be observed directly as functions of position on the solar disk as well as time. Thus here it is possible to analyze their spatial properties. This is done by means of a generalized 2-dimensional Fourier transform in position on the solar surface, to isolate particular values of l and m. This is followed by a Fourier transform in time which isolates the frequencies of the modes of that type. In fact, the average over the stellar surface implicit in observations of stellar oscillations can be thought of as one example of such a spatial Fourier transform.
Note that the oscillation data, rather than a continuous function, amount to values constrained by experimental error evaluated at a grid of positions and times. When computing transforms, values of this "function" outside this grid have to be interpolated and the integrals approximated by finite sums, a process inevitably introducing further errors. Details of the numerical methods used are included with the transformed data for purposes of comparison and constraining errors.
This discussion is adapted from the Jørgen Christensen-Dalsgaard lecture notes on stellar oscillations.^{[15]}
Information about helioseismic waves (such as mode frequencies and frequency-splitting) collected by transforming the oscillation data can be used to infer numerical details of internal features of the Sun such as the internal sound speed and the internal differential rotation. Equations and analytic relations such as integrals can be manipulated to relate the desired internal properties to the transformed data. The numerical methods used are adapted to the particular internal features examined so as to extract the maximum amount of information, with the least error, from the oscillations about the internal features. This process is termed helioseismic inversion.
As an example in slightly more detail, the oscillation frequency splitting can be related, via an integral, to the angular velocity within the sun.^{[15]}
Helioseismic observations reveal the inner uniformly rotating zone and the differentially rotating envelope of the Sun, roughly corresponding to the radiation and convection zones, respectively.^{[3]} See the diagram on the right. The transition layer is called the tachocline.
The age of the sun can be inferred with helioseismic studies.^{[16]} This is because the propagation of acoustic waves deep within the sun depends on the composition of the sun, in particular the relative abundance of helium and hydrogen in the core. Since the sun has been fusing hydrogen into helium throughout its lifetime, the present day abundance of helium in the core can be used to infer the age of the sun, using numerical models of stellar evolution applied to the Sun (Standard solar model). This method provides verification of the age of the solar system gathered from the radiometric dating of meteorites.^{[17]}
The goal of local helioseismology, a term first used in 1993,^{[18]} is to interpret the full wave field observed at the surface, not just the mode (more precisely, eigenmode) frequencies. Another way to look at it, is that global helioseismology studies standing waves of the entire Sun and local helioseismology studies propagating waves in parts of the Sun. A variety of solar phenomena are being studied, including sunspots, plage, supergranulation, giant cell convection, magnetically active region evolution, meridional circulation, and solar rotation.^{[19]} Local helioseismology provides a three-dimensional view of the solar interior, which is important to understand large-scale flows, magnetic structures, and their interactions in the solar interior.
There are many techniques used in this new and expanding field, which include:
This section is adapted from Laurent Gizon and Aaron C. Birch, "Local Helioseismology", Living Rev. Solar Phys. 2, (2005), 6. online article (cited on November 22, 2009).
An internal jet stream moving behind schedule may explain the delayed start to the solar cycle in 2009.^{[29]}
Chlorine, Protostar, Stellar structure, Peer review, Solar System
United Kingdom, Australia, Electronics, California, Spain
Sun, Solar System, Chromosphere, Palo Alto, California, University of Sheffield
Asteroseismology, EChO, European Space Agency, Kepler (spacecraft), Spitzer Space Telescope
Solar cycle, Star, Trace, Solar and Heliospheric Observatory, Solar System