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Science From BiSON. Key Science Themes. Structure of the Deep Radiative Interior Sound Speed and Rotation. Origin and Influence of Solar Cycle. Origins of the Oscillations Mode excitation and damping; surface physics. Solar Mean Magnetic Field (SMMF). …Roger New & Balazs Pinter.
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Key Science Themes • Structure of the Deep Radiative Interior • Sound Speed and Rotation • Origin and Influence of Solar Cycle • Origins of the Oscillations • Mode excitation and damping; surface physics • Solar Mean Magnetic Field (SMMF) …Roger New & Balazs Pinter
Achieving our Goals • Specific Investigations • Many in collaboration • Lots of connectivity between investigations • Over-arching data preparation and analysis tasks
Over-arching Tasks • Data calibration • Modelling/removal low-frequency footprint • Optimisation of data selection • Data preparation • Time series construction
Time series construction Knitting a week of data together 10 hr 2 m/s Residual velocity (m/s) Time
Over-arching Tasks • Data calibration • Modelling/removal low-frequency footprint • Optimisation of data selection • Data preparation • Time series construction • Gap filling • Public dissemination of data
Over-arching Tasks • Mode parameter extraction • Development of fitting techniques
Changes Across the Mode Spectrum Low Frequency High Frequency l=2/0 mode pairs in BiSON data
Over-arching Tasks • Mode parameter extraction • Development of fitting techniques • Development and application of artificial data • Monte-Carlo applications vital for testing analysis(at all stages…)
Key Science Themes • Structure of the Deep Radiative Interior • Origin and Influence of Solar Cycle • Origins of the Oscillations • Solar Mean Magnetic Field (SMMF)
Structure of the Deep Radiative Interior • Sound speed and rotation profiles • New modes at low frequencies • More accurate frequency extraction • Removal of effects of surface layers, i.e., peak and multiplet asymmetry, solar-cycle shifts • Comparative/correlation analyses of different data vital
Origin and Influence of Solar Activity Cycle • Study of mode parameter variations in greater detail • Dependence on angular degree, l Dependence on frequency • Careful comparison between datasets • What do differences between sets tell us? • Inform models of variations in mode properties
Origins of the Oscillations • Mode excitation and damping • Using observation to inform models • Origin of large or unusual excitations: linking the interior to the surface • Tracking mode phase as an important tool
Origins of the Oscillations • Surface Physics • Resonant peak asymmetry and phase shifts: influence of granulation • Height dependence in photosphere • SMMF
Solar Cycle Variations Chaplin et al., in preparation Cycle 23 Cycle 22
Solar Cycle Variations Howe et al., 2003, ApJ, 588, 1204 Frequency BiSON GONG Power density Linewidth
An Unusual Excitation that Bucks the Long-Term Trend What was the cause? Chaplin et al., 2003, ApJ, L582, 115
Needles in a Haystack: Modes at Low Frequencies Predicted 9 years of BiSON data
Low-Frequency p Modes Chaplin et al., 2002, MNRAS, 336, 979
Importance of removal of surface activity Inversion for sound speed with fractional radius 0.002 ...with ‘raw’ BiSON frequencies 0.001 -0.001 -0.002 0.2 0.4 0.6 0.8 1.0 Inversions courtesy A. Kosovichev
Importance of removal of surface activity Inversion for sound speed with fractional radius 0.002 ...with ‘corrected’ BiSON frequencies 0.001 -0.001 -0.002 0.2 0.4 0.6 0.8 1.0 Inversions courtesy A. Kosovichev
Rotation Inversions Effect of adding more low-l splittings at low frequency Artificial data: 400 nHz input
Low-Frequency p Modes BiSON minus SACLAY model frequencies Chaplin et al., 2002, MNRAS, 336, 979
Frequency Uncertainties Chaplin et al., 2002, MNRAS, 330, 731
Low-Frequency p Modes GOLF minus BiSON frequencies Chaplin et al. 2002, 336, 979; Bertello et al., 2000a, b
Frequency Uncertainties Scale as T½ Perform analysis to find for model where errors scale as T Chaplin et al., 2002, MNRAS, 330, 731
Mode Lifetimes Chaplin et al., 2002, MNRAS, 330, 731
High Frequency Spectrum Solid: GOLF Dashed: BiSON
High-Frequency Peaks GOLF blue wing minus BiSON
Low-Resolution BiSON Spectrum Gear-frequency artefact
l=2 Multiplet Frequency Asymmetries No magnetic field Now apply B field... Power m =0 Frequency m =+2 m =-2
l=2 Multiplet Frequency Asymmetries Pattern becomes asymmetric Power m =0 Frequency m =+2 m =-2
l=2 Multiplet Frequency Asymmetries Pattern asymmetry given by: Power an m =0 Frequency m =+2 m =-2
l=2 Multiplet Frequency Asymmetries GOLF BiSON Chaplin et al., MNRAS, in press
l=2 Multiplet Frequency Asymmetries Chaplin et al., MNRAS, in press
l=2 Multiplet Frequency Asymmetries BiSON: asymmetric minus symmetric multiplet model frequency 864-d data set
Low-l Peak Asymmetries BiSON: asymmetric- minus symmetric-peak model frequency 864-d data set
Rotational Splittings (Synodic) Chaplin et al., 2001, MNRAS, 327, 1127
Impact of Fitting Model Different assumed component height ratios cf. Chaplin et al., 2001, MNRAS, 327, 1127
Sidereal Splittings from 3456-d spectrum Median 431.8 2.7 nHz Unweighted 430.5 2.8 nHz Weighted 430.1 1.2 nHz