info:objective
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| + | ======= Objective of the WP ======= | ||
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| + | The objectives of this WP are: | ||
| + | - To find out how to get accurate matches between observed and theoretical frequencies computed for the PLATO pipelines | ||
| + | - To find the right oscillation code for the theoretical frequencies computation | ||
| + | - Provide a version of the code to be used in the pipeline | ||
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| + | ^Current frequency precision (2019)| | ||
| + | |:!: 0.1 μHz (around υ_max)| | ||
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| + | ===== ESTA/CoRoT (2008) Precision results ===== | ||
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| + | Summary of the oscillation frequency comparison results **[[[data: | ||
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| + | ^Conclusions ^ Comment | | ||
| + | |1 | 4K yields 0.02μHz precision, 2K yields 0.5 μHz precision (in average). | ||
| + | |2 | 2K does not properly distribute mesh points in the boundaries of the BV, 4K has no those problems | | ||
| + | |3 | O(2)+Richardson Extrapolation indistinguishable from O(4) neither for 4K nor for 2K| | ||
| + | |4 | r or r/P as integration variable may introduce errors if G is not consistent| | ||
| + | |5 | Eulerian P / Lagrangian P as eigenfunction (modifies BV frequency, euP). May have an impact if thermodynamical quantities are not internally consistent (e.g. OPAL tables) | | ||
| + | |6 | 2K not adequate for large/small separations. 4K yields frequency differences below obs precision| | ||
| + | |7 | Proper sampled BV is key to avoid numerical bias. 4K partially overcome the problem| | ||
| + | |8 | G constant inconsistencies affect the frequencies comparison (up to 0.3-0.4 μHz !). Should be taken from the model| | ||
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