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Present accuracies in spectroscopic chemical abundances

” These things … were not discovered by philosophy or the arts of reason , but by chance . …. There are still many things of excellent use , stored up in the lap of nature , … lying quite out of the path of imagination .”

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Present accuracies in spectroscopic chemical abundances

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  1. ”Thesethings … were not discovered by philosophy or the arts ofreason, but by chance. …. Thereare still manythingsof excellent use, storedup in the lapofnature, … lyingquiteoutof the pathofimagination.” Francis Bacon, NovumOrganum (1620)

  2. Present accuracies in spectroscopicchemicalabundances • Rarelybetterthan 0.1 dex (evenrelatively) • Some ~0.01 dex. What do welearnfrom those?

  3. Solar composition not normal for solar-type stars Meléndez et al. (2009) ≈0.08 dex≈20% Birth environment? Effects of planets? Not full mixing?

  4. Present accuracies in spectroscopicchemicalabundances • Rarelybetterthan 0.1 dex (evenrelatively) • ~0.01 dex in special casesonly. Whatare the problems? • Obs. data: Blends, continua • Fundamental parameters: Teff, log g, mass, radius, distance, extinction, … • Modelling: Atomic data, non-LTE, convection, … • Interpretation: What do atmosphericabundancesrepresent? Solution: Fit realistic and physicallyconsistent 3D NLTE, MHD modelstoadequateobservables. (Anyotherdecentways??)

  5. The multi-D world of stars And there are more: , B, d/dt of all of the above.  Stars contain a wealth of information about themselves, their planetary systems and their birth environments Gilmore et al. (2012), The Messenger

  6. The many Ds of hi-res instrumentation • Wavelengthcoverage • Resolving power • Achievable signal-to-noise ratio • Various calibrational needs • Stability • Multiplexing • Polarimetry • ... Can we have it all in one instrument?

  7. Wavelengthcoverage: Spectrallines and continua GJ 849 (M 3.5 V) Heiteret al. (2012) YCVn (C 5,4) UUAur(C 5 II) Lambert et al. (1986) J-band Satisfactorycontinua for M stars J-band K-band ”Quasicontinua”for C stars CO 1st overtone offers diagnostics on structure and dynamics Note: unidentifiedlines! Near IR useful for cool stars … butmanyunidentifiedlines as yet.

  8. Spectral resolution:Line profilesfor convection, rotation, magneticfields, … Ramírez et al. (2010): HD 122563

  9. Line profilesfor convection, rotation, magneticfields, … Gray & Brown (2006): Arcturus Resolve the spectrafully!

  10. Achievable S/N NGC 6752 @ [Fe/H]=-1.6: Ca, Sc, Ti and Fe NGC 6397 @ [Fe/H]=-2.1 Korn et al. (2006, 2007) Nordlander et al. (2012) TOP stars: 30 h with FLAMES-UVES S/N  35 per rebinned pixel Gruyters et al. (2012)

  11. Blaze correction reliability cf. Korn (2002) More generally: why accept calibrations thatare ”astronomical” rather thanphysical? amplitude ≥5%!

  12. Physicalcalibrationofspectrometer See Stubbs & Tonry (2012): arXiv1206.6695: Addressing the PhotometricCalibrationChallenge: Explicit determination of the Instrumental Response and AtmosphericResponseFunctions, and Trying it All Together.

  13. (Spectro)photometry Teffto 50K => B-V to 0.01 or V-K to 0.03 mag. or correspondingaccuracy in spectrophotometric gradients. Problem: Variable stars! Simultaneous data needed.

  14. Polarization With a 1‰ accuray in polarization meanfieldsofabout 100 Gauss shouldbe measurable => 0.03 dexin abundance (betterwith IR linesobserved!) SeeFabbian et al. (2010)

  15. Our CODEX: No SIMPLE compromises! E-ELT instrumentation: second to none

  16. So: Do new things! • Look deeper! • Go for higher resolution and S/N! • Explore new wavelength regions! • Takecontrolofcalibrations! • Investinto extra dimensions like polarization …

  17. Time resolution Cieslinski et al. (2010): Polar (AM Her star) RBS 0324 15 min intervals. Muchhigherfrequencyrequires special measures. HdHeII Hb

  18. Achievable S/N • S/N per unit time time domain ever more important ability to study ever shorter phenomena limited by the light collecting power and the read-out time Barclay et al. (2011)

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