L-NU Diagrams

An MDI Medium-l Power Spectrum (l-nu Diagram)
Produced by Alexander Kosovichev, SOI Team, Stanford.

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The Sun resonates like a huge musical instrument. The pitch of the resonance depends on the physical conditions in the interior of the Sun where the sound waves travel. The path the sound waves take also determines the spatial pattern the resonant modes of oscillation display at the solar surface.

The figure shows how much acoustic energy there is at each frequency for every one of the spatial modes of oscillation. Unlike a musical instrument that is tuned to a single frequency and a few harmonious overtones, the Sun resonates in tens of millions of ways all at the same time. The frequency, often called nu, of each mode reveals something about a slightly different part of the Sun's interior. The spatial modes are identified from patterns on the dopplergrams that are made each minute.

The frequencies are very low compared to sound waves we are used to hearing. Most of the power (shown in yellow) is concentrated in a band near 3 mHz, that's one oscillation every 5 minutes. Sound waves we can hear vibrate from tens to thousands of times per second. Modes with higher frequencies aren't trapped inside the Sun, so they don't resonate. Modes with lower frequencies are so quiet it is hard to pick them out of the background noise.

An l-nu diagram from an MDI 8-hour campaign of high resolution Doppler images. Produced by Jesper Schou, SOI Team, Stanford.

The spatial scale of the modes is indicated by the angular degree, l, and tells how many node lines there are in the pattern at the surface of the Sun. The l=0 modes are 'breathing' modes where the whole surface of the Sun moves in and out at the same time. Higher order modes divide the surface into a pattern like a checker board, where adjacent squares move in different directions at any give time. The higher the degree the smaller the spatial scale. The modes are described by mathematical funcations called spherical harmonics. A mode of a particular degree, l, at the surface can be associated with resonances having any number of nodes in the radial direction inside the Sun. The number of radial nodes is called the mode's order. The curved lines in the figure are associated with different radial orders. For a given order (along one of the curved lines) the frequency increases with increasing spatial degree. For a given degree, the frequency increases with order. In the figure, the lower left corner is most closely related to what is happening in the core of the Sun. Moving up in frequency or degree tells more about what is happening near the surface.

Each of the lines is fairly broad. That's because sound waves of a particular degree can travel in different directions. Actually there are 2*l + 1 modes for each angular degree (and each order) corresponding to slightly different directions of travel. [For example, that would be 301 modes for l=150 on each line.] If the material through which any of these modes is traveling is moving, that affects the measured frequency of the mode. The rotation of the Sun causes the biggest frequency shift and makes the lines shown in the figure broad. Other motions within the Sun along the path taken by the waves cause different types of frequency changes. Analysis of these frequency changes reveals the internal motions of the Sun.

The faint line at lowest frequency is actually a different kind of wave, very much like ocean waves. It tells only about what is happening at the surface of the Sun.



The l-nu (period versus wavelength) diagram determined from observations made by the MDI instrument during a continuous 83-hour observing run in April 1996. The x axis is the inverse spatial wavelength, with the right end representing waves on the order of 10,000 km (l=400). The y axis represents the mode frequency up to the instrument Nyquist cutoff (2 minutes or 0.00833 Hz). Produced by Rock Bush, SOI Team, Stanford.


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This page is http://solar-center.stanford.edu/explainlnu.html
© 2007 Stanford University. All rights reserved.
Last revised by JTH on Sept 12, 1997