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Phase Time and Envelope Time in Time-Distance Analysis and Acoustic Imaging

Author
Wang, Gwo-Ping
Published
[1999].
Physical Description
1 electronic document
Additional Creators
Marquette, William, Jimenez, Antonio, Landenkov, Oleg, Ai, Guoxiang, Goode Philip, Rabello-Soares, Maria Cristina, Sun, Ming-Tsung, Chang, Hsiang-Kuang, Chou, Dean-Yi, Duvall, Thomas Lee, and Ehgamberdiev, Shuhrat
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Summary
Time-distance analysis and acoustic imaging are two related techniques to probe the local properties of solar interior. In this study, we discuss the relation of phase time and envelope time between the two techniques. The location of the envelope peak of the cross correlation function in time-distance analysis is identified as the travel time of the wave packet formed by modes with the same w/l. The phase time of the cross correlation function provides information of the phase change accumulated along the wave path, including the phase change at the boundaries of the mode cavity. The acoustic signals constructed with the technique of acoustic imaging contain both phase and intensity information. The phase of constructed signals can be studied by computing the cross correlation function between time series constructed with ingoing and outgoing waves. In this study, we use the data taken with the Taiwan Oscillation Network (TON) instrument and the Michelson Doppler Imager (MDI) instrument. The analysis is carried out for the quiet Sun. We use the relation of envelope time versus distance measured in time-distance analyses to construct the acoustic signals in acoustic imaging analyses. The phase time of the cross correlation function of constructed ingoing and outgoing time series is twice the difference between the phase time and envelope time in time-distance analyses as predicted. The envelope peak of the cross correlation function between constructed ingoing and outgoing time series is located at zero time as predicted for results of one-bounce at 3 mHz for all four data sets and two-bounce at 3 mHz for two TON data sets. But it is different from zero for other cases. The cause of the deviation of the envelope peak from zero is not known.
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Collection
NASA Technical Reports Server (NTRS) Collection.
Note
Document ID: 20000017990.
Terms of Use and Reproduction
No Copyright.
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