2008
DOI: 10.1002/asna.200710977
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A framework for describing correlated excitation of solar p‐modes

Abstract: In a previous paper we suggested that, for a given p mode, the excitation function is the same as the component of the solar background noise that has an identical surface spherical harmonic projection (over the corresponding range of temporal frequency). An important consequence of this surmise is that the excitation of overtones of a given angular degree and azimuthal order will be correlated in time. In this note, we introduce the basic principles and a mathematical description of correlated mode excitation… Show more

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Cited by 5 publications
(11 citation statements)
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“…Having fixed the input i s , we then used the tabulated v i sin s and asteroseismic radius to determine the input s n . The power spectra were directly generated in the frequency domain, having preserved the same frequency resolution as in the real data and properly modeled the correlation between the background noise and the excitation function (see Chaplin et al 2008). The adopted mode linewidths and S/N were based on the observed linewidths and S/N of radial modes (not split by rotation).…”
Section: Appendix C Tests With Artificial Datamentioning
confidence: 99%
“…Having fixed the input i s , we then used the tabulated v i sin s and asteroseismic radius to determine the input s n . The power spectra were directly generated in the frequency domain, having preserved the same frequency resolution as in the real data and properly modeled the correlation between the background noise and the excitation function (see Chaplin et al 2008). The adopted mode linewidths and S/N were based on the observed linewidths and S/N of radial modes (not split by rotation).…”
Section: Appendix C Tests With Artificial Datamentioning
confidence: 99%
“…This can be understood by considering the analogy of damped, stochastically forced oscillators. Modes of different frequencies will be 'kicked' by the common excitation at different phases in their oscillation cycles, and provided the frequencies differ by more than a few line widths (see Chaplin et al 2008) -a condition easily met by consecutive overtones of the low-l modes, which are separated by ∼ 135 µHz -there will be significant differences in how the amplitudes vary in time, due to the excitation.…”
Section: Correlated Noise and Mode Excitationmentioning
confidence: 99%
“…APPENDIX A: THE SOLARFLAG COMPLEX FREQUENCY AMPLITUDE, AND FREQUENCY POWER, SPECTRUM In the following description -which is based on the detailed discussions in Toutain et al (2006) Chaplin et al (2008) -we model the p-modes as forced, damped oscillators having a high Q. The frequency response of a given mode (with n, l and m) is then just a Lorentzian, which may be written in complex amplitude form as:…”
mentioning
confidence: 99%
“…First, background noise is correlated with the excitation functions of the modes. Secondly, overtones of the same angular degree and azimuthal order have excitation functions that are correlated in time (see Chaplin, Elsworth & Toutain 2008a). In this framework, correlation of the excitation follows naturally from invoking correlations with the background noise.…”
Section: Introductionmentioning
confidence: 99%