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Neon and oxygen in stellar coronae
       A unification with the Sun


            Jan Robrade

         Hamburger Sternwarte

From Atoms to Stars, July 2011, Oxford
Overview



1   Neon and the solar modeling problem


2   Data and measurements


3   X-ray properties of weakly active stars


4   Coronal Ne/O ratios
Why care?

 The chemical composition of the Sun is one of the most important
 yardsticks in astronomy with implications for basically all fields
 from planetary science to the high-redshift Universe.
 (Asplund, Grevesse, Sauval 2005)




Jan Robrade (Hamburger Sternwarte)   Ne/O in stellar coronae   26.07.2011   3 / 28
Our star - the Sun
 The ideal world
        Abundances from Grevesse & Sauval, 1998
        Solar interior model
        Agreement with helioseismologic measurements

 Trouble in paradise?
        Revised abundances by Asplund+ 2005
             sophisticated 3D hydrodynamic modelling
             high quality atomic line data, includes non-LTE calculations
             reduced abundances of C, N, O by 30 – 40%
             better agreement e.g. with ISM measurements
             but:
             significant disagreement with helioseismology
             missing opacity

 Way out needed!
Jan Robrade (Hamburger Sternwarte)   Ne/O in stellar coronae          26.07.2011   4 / 28
Neon and oxygen

 Increase neon by a factor of 3 – 4 !!               (e.g. Antia & Basu 2005, Bahcall 2005)




 Why neon?

        no photospheric lines in solar spectrum
        no useful meteorite data (noble gas, volatile)
        very common element
        strong source of opacity
        determined indirectly
             coronal and/or TR lines
             solar wind/energetic particles
             oxygen as reference element; determine ANe /AO (Ne/O)
        AGS05: Ne/O = 0.15 quite low (same as AnGr89)

Jan Robrade (Hamburger Sternwarte)   Ne/O in stellar coronae                            26.07.2011   5 / 28
The controversy




 ’The solar modelling problem solved
 by the abundance of neon in nearby
 stars’                                             top: solar corona - active regions
 Ne/O = 0.41 (Drake & Testa, 2005)                  Ne/O = 0.18 (Schmelz et al. 2005)
 mainly active stars                                bottom: transition region - quiet sun
 objections from solar observers                    Ne/O = 0.17 (Young 2005)


Jan Robrade (Hamburger Sternwarte)   Ne/O in stellar coronae                  26.07.2011    6 / 28
Ne/O in the Sun




 A short history of solar Ne/O ratios:
        0.21 (0.16-0.31) solar corona           (Acton et al. 1975)

        0.17 (0.15-0.19) solar wind          (von Steiger & Geiss 1989)

        0.18 (0.15-0.22) Sun         (Grevesse & Sauval 1998)

 transient deviations in individual flares observed, but in general:

   Ne/O ≈ 0.2 - independent of atmospheric layer and activity phase!

Jan Robrade (Hamburger Sternwarte)      Ne/O in stellar coronae           26.07.2011   7 / 28
Ne/O in inactive stars




 Sun   (von Steiger & Geiss 1989)                 α Centauri A   (Raassen+ 2003)
 solar wind/energetic particles
                                                  X-rays/corona
 TR/corona      (Feldman 1992)


  Chemical fractionation Pt. I
         fractionation occurs in chromosphere
         weakly active stars show FIP-effect
         O and Ne are high FIP elements ⇒ Ne/O ratio unchanged
Jan Robrade (Hamburger Sternwarte)   Ne/O in stellar coronae                       26.07.2011   8 / 28
Ne/O in active stars




 HR 1099 (Brinkman+ 2001)                         active M dwarfs   (Robrade+ 2005)

 X-rays/corona                                    X-rays/corona

  Chemical fractionation Pt. II
         highly active stars show IFIP-effect
         strength depends on activity level
         Ne/O ratio changed
Jan Robrade (Hamburger Sternwarte)   Ne/O in stellar coronae                    26.07.2011   9 / 28
Neon and oxygen in weakly active stars


 Study coronal Ne/O of in a sample of stars similar to the Sun!


 Neon and oxygen in low activity stars                         (Robrade+ 2008; Robrade & Schmitt 2009)



 The sample:
 Altair (A7), Procyon (F5), β Com (G0), α Cen (G2+K1), HD 81809
 (G2+G9), Eri (K2), 61 Cyg (K5+K7)

        broad range of effective temperatures
        low to moderately active stars; log LX /Lbol = −5... − 7
        coronae dominated by cool plasma (T                    5 MK)
        Ne/O from emission line ratios + global modeling


Jan Robrade (Hamburger Sternwarte)   Ne/O in stellar coronae                         26.07.2011    10 / 28
Ne/O - emission line ratios

 Method I - emission line ratios
        strong emission lines from oxygen and neon (fitted with CORA)
        covered by XMM-Newton (RGS) and Chandra (LETGS)
        virtually free of blends
        well determined atomic data

 Construct ’temperature-independent’ line ratios:
        1975: O viii vs. Ne ix       (Acton, Catura, Joki, 1975)


 Used lines:
 O vii r (21.6 ˚), O viii Lyα (18.97 A), Ne ix r (13.45 ˚), Ne x Lyα (12.13 ˚)
               A                     ˚                  A                   A

        O viii vs. Ne ix + 0.15 Ne x          – energy flux weighting    (Drake & Testa, 2005)

        0.67 O viii - 0.17 O vii vs. Ne ix + 0.02 Ne x              - photon f. w.   (Liefke & Schmitt, 2006)




Jan Robrade (Hamburger Sternwarte)        Ne/O in stellar coronae                       26.07.2011      11 / 28
Ne/O - emission line ratios




                                                   Summed and scaled residuals of the
                                                   emissivities ≡ flat EMD).
   Theoretical emissivity curves for Ne            (CHIANTI 5, Landi+ 2006)
   and O and respective residuals.

        residuals smooth out only if EMD is very broad
        significant error for very cool stars possible
        L&S - too much neon, D&T - EM dependent trend


Jan Robrade (Hamburger Sternwarte)   Ne/O in stellar coronae              26.07.2011   12 / 28
Ne/O - spectral modeling



 Method II -’global’ modeling
        fit spectra with multi-temperature VAPEC models in XSPEC
        free abundances of Ne, O, Fe         (+ additional, if S/N sufficient)

        RGS/MOS or LETGS spectra
        check with Ne+O dominated spectral regions                                    ˚
                                                                       (11-14 + 18-23 A)

        include LETGS long-wavelength regime                   (85-100 ˚) - ’cooler’ Ne vii + viii
                                                                       A

        derive X-ray luminosities, coronal temperatures, Ne/O ratios
        absolute abundances more uncertain - EM interdependence




Jan Robrade (Hamburger Sternwarte)   Ne/O in stellar coronae                       26.07.2011   13 / 28
Ne/O - X-ray CCD spectra



                                                              NeX




                                     OVII
                                            OVIII
                                                       NeIX




 MOS CCD spectra of              Eri (black) and Procyon (red) with line features labeled




Jan Robrade (Hamburger Sternwarte)                  Ne/O in stellar coronae   26.07.2011   14 / 28
Ne/O - X-ray grating spectra




                                                           High resolution X-ray spectra
                                                           from XMM-Newton and
                                                           Chandra
                                                           good data quality obtained
                                                           Ne ix line most crucial




 Spectra of        Eri (LETGS) and 61 Cyg (RGS, co-added)
Jan Robrade (Hamburger Sternwarte)   Ne/O in stellar coronae               26.07.2011   15 / 28
X-ray data & coronal properties


         Star                        Mission    Obs.(No Exp.)       log LX    Tav.   LX /Lbol
                                                (ks)                (erg/s)   (MK)   log
          Eri (K2)                   XMM        13 (1)              28.2      3.8    -4.9
         HD 81809 (G2+G9)            XMM        72 (7)              28.7      4.0    -5.6
         61 Cyg (K5+K7)              XMM        103 (11)            27.3      3.2    -5.6, -5.5
         β Com (G0)                  XMM        41 (1)              28.2      3.4    -5.6
                                     Chandra    105 (1)
         Procyon (F5)                XMM        138 (3)             27.9      1.9    -6.5
                                     Chandra    139 (2)
         α Cen (G2+K1)               XMM        73 (9)              27.1      2.2    -7.3, -6.2
                                     Chandra    79 (1)
         Altair (A7)                 XMM        130 (1)             27.1      2.3    -7.4

 data taken 1999-2007 , XMM/RGS binary data unresolved
 MOS/RGS spectral fit for basic parameter, LX in 0.2 – 3.0 keV band



Jan Robrade (Hamburger Sternwarte)        Ne/O in stellar coronae                    26.07.2011   16 / 28
Results - weakly active stars




                  (Hempelmann 2006, Robrade+, in prep.)



  Global X-ray properties Pt. I
         all coronae are cool, av. TX ≈ 2 − 4 MK
         weak to minor contribution of 5 – 10 MK plasma
         FIP effect in the lesser active stars (α Cen, β Com)
         weak/no FIP effect in in moderately active stars
         many weakly active G and K dwarfs show cyclic X-ray activity

Jan Robrade (Hamburger Sternwarte)            Ne/O in stellar coronae   26.07.2011   17 / 28
Results - Altair




 XMM-observation of Altair            (Robrade & Schmitt, 2009)

        A7 star,     Teff ≈ 7800 K, M = 1.8 M , Vsini ≈ 220 km/s, i ≈ 60◦ , X-ray source

        X-ray properties similar to inactive sun
               LX = 1.4 × 1027 erg/s, log LX /Lbol = −7.4, 1 – 4 MK plasma
               minor activity, rotational modulation, long term stable
               solar-like abundances and FIP effect

 ’classical interpretation’: thin outer convective layer
Jan Robrade (Hamburger Sternwarte)      Ne/O in stellar coronae              26.07.2011   18 / 28
Results - Altair II

                                                      Altair - rotationally deformed
                                                              Vrot 60% breakup-speed ⇒
                                                              X-ray saturation level very low
                                                              oblate, axial ratio of a / b ≈ 1.1 – 1.2
                                                              gravity darkening ⇒ Teff range:
                                                              6900 K (equator) up to 8500 K (poles)
                                                              O vii f /i-ratio high:
                                                              tracer of density and UV-field
                                                              surface features at Teff 7400 K
                  CHARA (Monnier et al. 2007)

                                                                 f /i = R0 /(1 + φ/φc + ne /nc )
                                                                  (e.g. Gabriel & Jordan 1969, Porquet+ 2001)


  =⇒ Equatorial bulge corona

Jan Robrade (Hamburger Sternwarte)              Ne/O in stellar coronae                           26.07.2011    19 / 28
Neon and oxygen - results

  Global modeling - results
         Ne/O ratio robust

  Neon and oxygen line measurements
         virtually all lines detected in all stars
         few Ne x U.L. in LETGS spectra of coolest coronae
         account for Fe xvii blend in Ne x via emissivities (20 %)
         neglect Fe xix blends in Ne ix – low TX
         overall good agreement between multiple observations
                obs.-time average for cyclic stars
         Ne/O ratios - D&T vs. L&S
                similar for the hotter stars
                discrepancies for the coolest stars

Jan Robrade (Hamburger Sternwarte)    Ne/O in stellar coronae    26.07.2011   20 / 28
Ne/O - results I




 Coronal stellar Ne/O ratios and the ’classical’ Sun             (Robrade & Schmitt, 2009)

 (global fit: diamonds/solid line, D&T asterisks/dotted line, L&S squares/dashed line)


  Stellar X-ray data suggests Ne/O at upper bound of solar range


Jan Robrade (Hamburger Sternwarte)    Ne/O in stellar coronae                   26.07.2011   21 / 28
Ne/O - results II


 Ne/O ratios of individual stars
        Ne/O: 0.35 – 0.40 for Eri (0.37), 61 Cyg (0.36), HD 81809 (0.36)
        Ne/O: 0.25 – 0.35 for β Com (0.25), α Cen B (0.26)
        Ne/O: 0.20 – 0.25 for Procyon (0.22), α Cen A (0.21), Altair (0.20)

        overall good agreement with literature
        mod. active stars
                 Eri   (Wood & Linsky Ne/O = 0.36, Sanz-Forcada+ Ne/O = 0.4)
        weakly active stars
               Procyon (Raassen+ Ne/O = 0.22 , Sanz-Forcada+ Ne/O = 0.40)
               α Cen A/B (Raassen+ A: Ne/O = 0.18, B: Ne/O = 0.26, L&S Ne/O = 0.27)




Jan Robrade (Hamburger Sternwarte)      Ne/O in stellar coronae            26.07.2011   22 / 28
Ne/O - results III


 Ne/O ratios of stellar coronae
        coronal Ne/O ratio increases with activity in weakly active stars
               trend independent of analysis method
               trend independent of spectral type
        Ne/O ≈ 0.2 at log LX /Lbol ≈ −6.5
        Ne/O ≈ 0.4 at log LX /Lbol ≈ −4.5
        solar values typical for low activity stars
        Ne/O apparently saturates at higher activity levels
        larger datasets required to reveal details of chemical fractionation
               shape of ratio-curve
               dependence on sp. type, LX /Lbol vs. TX



Jan Robrade (Hamburger Sternwarte)   Ne/O in stellar coronae      26.07.2011   23 / 28
Solar modeling problem: further insights

 Other abundance determinations:
        low Ne/O ratio in photospheric study of early B stars       (Przybilla et al. 2008)

        Ne/O= 0.21 (0.19-0.23)       (absolute values intermediate to GS98 & AGS05)

        homogeneous distribution of elemental abundances in solar neighborhood



 Solar abundances revised (Asplund+ 2009)
        slightly higher solar metallicity (+ 10%)
        Ne/O = 0.17 (0.14-0.22)
        absolute abundances of Ne and O:
        agreement between Sun, B stars and H ii-regions within errors
        Lodders+ 2009, Ne/O = 0.21


Jan Robrade (Hamburger Sternwarte)     Ne/O in stellar coronae                 26.07.2011     24 / 28
Caveats & open Questions


                                                   Measured and predicted sound speed
                                                   (Asplund+ 2009)



                                                   Discrepancy to helioseismology
                                                   alleviated but still significant!


        Solar problems
               sound speed profile wrong
               convection zone depth too shallow
               interior He abundance too low
        Possible solutions
               revise abundance calculations
               revise opacity calculations for solar interior
               revise diffusion model - interior is more metal rich
               internal gravity waves - promising, but only qualitatively evaluated
Jan Robrade (Hamburger Sternwarte)   Ne/O in stellar coronae              26.07.2011   25 / 28
Caveats & open Questions II


 Chemical fractionation:
        cause of fractionation not fully explained
        transition: FIP- no-FIP - IFIP
        Laming-models promising (ponderomotive force)
        activity good tracer - importance of fundamental parameter
        elements: charge, mass
        stars: gravity, temperature gradients, radiation, electric & magnetic fields
        details of abundance trends need to be refined
        other elements need to be considered




Jan Robrade (Hamburger Sternwarte)   Ne/O in stellar coronae          26.07.2011   26 / 28
Summary



 Neon and oxygen in stellar coronae
        Ne/O ratio depends on stellar activity
        Ne/O increases with activity in weakly to moderately active stars
        Ne/O ≈ 0.2 ± 0.05 in weakly active stars
        Neon is not the solution for the solar modelling problem




               The Sun is a typical star!

Jan Robrade (Hamburger Sternwarte)   Ne/O in stellar coronae       26.07.2011   27 / 28
Ne/O - line fluxes
 Measured line fluxes in 10−5 photons cm−2 s−1 from RGS or LETGS (C) and energy
 flux ratio of the O viii(Lyα) to O vii(r) line.

            Star              O vii(r)   O viii        Ne ix(r)    Ne x∗      O8/O7(r)
            61 Cyg            6.6±0.4    9.1±0.5       2.0±0.3     1.6±0.2    1.57±0.13
            Altair            4.9±0.4    3.7±0.3       0.4±0.1     0.2±0.1    0.86±0.10
            α Cen             33.5±1.3   27.0±1.2      4.1±0.5     1.6±0.2    0.92±0.05
            α Cen 03/04       47.9±2.1   45.4±1.5      5.5±0.8     2.4±0.5    1.08±0.06
            α Cen A (C)       9.2±1.0    3.2±0.5       0.5±0.3        0.2     0.40±0.07
            α Cen B (C)       11.5±1.0   6.3±0.6       1.3±0.4        0.2     0.62±0.08
            β Com             3.8±0.6    5.9±0.6       0.9±0.3     0.6±0.3    1.77±0.33
             Eri              44.1±2.6   78.0±3.0      21.2±2.4    10.5±1.4   2.01±0.14
             Eri (C)          41.5±1.6   78.9±1.7      18.8±0.9    16.7±0.9   2.16±0.10
            HD 81809          1.0±0.3    2.3±0.3       0.5±0.2     0.5±0.2    2.62±0.86
            Procyon           35.6±1.1   22.9±0.9      1.8±0.3     0.5±0.2    0.73±0.04
            Procyon (C)       29.1±1.6   17.3±1.0      2.5±0.5     0.7±0.3    0.68±0.05
            Procyon (C)       30.3±1.7   18.9±1.1      1.4±0.3        0.2     0.71±0.06
       ∗
           Blended with Fe xvii.


Jan Robrade (Hamburger Sternwarte)       Ne/O in stellar coronae                26.07.2011   28 / 28

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Neon and oxygen in stellar coronae - a unification with the Sun

  • 1. Neon and oxygen in stellar coronae A unification with the Sun Jan Robrade Hamburger Sternwarte From Atoms to Stars, July 2011, Oxford
  • 2. Overview 1 Neon and the solar modeling problem 2 Data and measurements 3 X-ray properties of weakly active stars 4 Coronal Ne/O ratios
  • 3. Why care? The chemical composition of the Sun is one of the most important yardsticks in astronomy with implications for basically all fields from planetary science to the high-redshift Universe. (Asplund, Grevesse, Sauval 2005) Jan Robrade (Hamburger Sternwarte) Ne/O in stellar coronae 26.07.2011 3 / 28
  • 4. Our star - the Sun The ideal world Abundances from Grevesse & Sauval, 1998 Solar interior model Agreement with helioseismologic measurements Trouble in paradise? Revised abundances by Asplund+ 2005 sophisticated 3D hydrodynamic modelling high quality atomic line data, includes non-LTE calculations reduced abundances of C, N, O by 30 – 40% better agreement e.g. with ISM measurements but: significant disagreement with helioseismology missing opacity Way out needed! Jan Robrade (Hamburger Sternwarte) Ne/O in stellar coronae 26.07.2011 4 / 28
  • 5. Neon and oxygen Increase neon by a factor of 3 – 4 !! (e.g. Antia & Basu 2005, Bahcall 2005) Why neon? no photospheric lines in solar spectrum no useful meteorite data (noble gas, volatile) very common element strong source of opacity determined indirectly coronal and/or TR lines solar wind/energetic particles oxygen as reference element; determine ANe /AO (Ne/O) AGS05: Ne/O = 0.15 quite low (same as AnGr89) Jan Robrade (Hamburger Sternwarte) Ne/O in stellar coronae 26.07.2011 5 / 28
  • 6. The controversy ’The solar modelling problem solved by the abundance of neon in nearby stars’ top: solar corona - active regions Ne/O = 0.41 (Drake & Testa, 2005) Ne/O = 0.18 (Schmelz et al. 2005) mainly active stars bottom: transition region - quiet sun objections from solar observers Ne/O = 0.17 (Young 2005) Jan Robrade (Hamburger Sternwarte) Ne/O in stellar coronae 26.07.2011 6 / 28
  • 7. Ne/O in the Sun A short history of solar Ne/O ratios: 0.21 (0.16-0.31) solar corona (Acton et al. 1975) 0.17 (0.15-0.19) solar wind (von Steiger & Geiss 1989) 0.18 (0.15-0.22) Sun (Grevesse & Sauval 1998) transient deviations in individual flares observed, but in general: Ne/O ≈ 0.2 - independent of atmospheric layer and activity phase! Jan Robrade (Hamburger Sternwarte) Ne/O in stellar coronae 26.07.2011 7 / 28
  • 8. Ne/O in inactive stars Sun (von Steiger & Geiss 1989) α Centauri A (Raassen+ 2003) solar wind/energetic particles X-rays/corona TR/corona (Feldman 1992) Chemical fractionation Pt. I fractionation occurs in chromosphere weakly active stars show FIP-effect O and Ne are high FIP elements ⇒ Ne/O ratio unchanged Jan Robrade (Hamburger Sternwarte) Ne/O in stellar coronae 26.07.2011 8 / 28
  • 9. Ne/O in active stars HR 1099 (Brinkman+ 2001) active M dwarfs (Robrade+ 2005) X-rays/corona X-rays/corona Chemical fractionation Pt. II highly active stars show IFIP-effect strength depends on activity level Ne/O ratio changed Jan Robrade (Hamburger Sternwarte) Ne/O in stellar coronae 26.07.2011 9 / 28
  • 10. Neon and oxygen in weakly active stars Study coronal Ne/O of in a sample of stars similar to the Sun! Neon and oxygen in low activity stars (Robrade+ 2008; Robrade & Schmitt 2009) The sample: Altair (A7), Procyon (F5), β Com (G0), α Cen (G2+K1), HD 81809 (G2+G9), Eri (K2), 61 Cyg (K5+K7) broad range of effective temperatures low to moderately active stars; log LX /Lbol = −5... − 7 coronae dominated by cool plasma (T 5 MK) Ne/O from emission line ratios + global modeling Jan Robrade (Hamburger Sternwarte) Ne/O in stellar coronae 26.07.2011 10 / 28
  • 11. Ne/O - emission line ratios Method I - emission line ratios strong emission lines from oxygen and neon (fitted with CORA) covered by XMM-Newton (RGS) and Chandra (LETGS) virtually free of blends well determined atomic data Construct ’temperature-independent’ line ratios: 1975: O viii vs. Ne ix (Acton, Catura, Joki, 1975) Used lines: O vii r (21.6 ˚), O viii Lyα (18.97 A), Ne ix r (13.45 ˚), Ne x Lyα (12.13 ˚) A ˚ A A O viii vs. Ne ix + 0.15 Ne x – energy flux weighting (Drake & Testa, 2005) 0.67 O viii - 0.17 O vii vs. Ne ix + 0.02 Ne x - photon f. w. (Liefke & Schmitt, 2006) Jan Robrade (Hamburger Sternwarte) Ne/O in stellar coronae 26.07.2011 11 / 28
  • 12. Ne/O - emission line ratios Summed and scaled residuals of the emissivities ≡ flat EMD). Theoretical emissivity curves for Ne (CHIANTI 5, Landi+ 2006) and O and respective residuals. residuals smooth out only if EMD is very broad significant error for very cool stars possible L&S - too much neon, D&T - EM dependent trend Jan Robrade (Hamburger Sternwarte) Ne/O in stellar coronae 26.07.2011 12 / 28
  • 13. Ne/O - spectral modeling Method II -’global’ modeling fit spectra with multi-temperature VAPEC models in XSPEC free abundances of Ne, O, Fe (+ additional, if S/N sufficient) RGS/MOS or LETGS spectra check with Ne+O dominated spectral regions ˚ (11-14 + 18-23 A) include LETGS long-wavelength regime (85-100 ˚) - ’cooler’ Ne vii + viii A derive X-ray luminosities, coronal temperatures, Ne/O ratios absolute abundances more uncertain - EM interdependence Jan Robrade (Hamburger Sternwarte) Ne/O in stellar coronae 26.07.2011 13 / 28
  • 14. Ne/O - X-ray CCD spectra NeX OVII OVIII NeIX MOS CCD spectra of Eri (black) and Procyon (red) with line features labeled Jan Robrade (Hamburger Sternwarte) Ne/O in stellar coronae 26.07.2011 14 / 28
  • 15. Ne/O - X-ray grating spectra High resolution X-ray spectra from XMM-Newton and Chandra good data quality obtained Ne ix line most crucial Spectra of Eri (LETGS) and 61 Cyg (RGS, co-added) Jan Robrade (Hamburger Sternwarte) Ne/O in stellar coronae 26.07.2011 15 / 28
  • 16. X-ray data & coronal properties Star Mission Obs.(No Exp.) log LX Tav. LX /Lbol (ks) (erg/s) (MK) log Eri (K2) XMM 13 (1) 28.2 3.8 -4.9 HD 81809 (G2+G9) XMM 72 (7) 28.7 4.0 -5.6 61 Cyg (K5+K7) XMM 103 (11) 27.3 3.2 -5.6, -5.5 β Com (G0) XMM 41 (1) 28.2 3.4 -5.6 Chandra 105 (1) Procyon (F5) XMM 138 (3) 27.9 1.9 -6.5 Chandra 139 (2) α Cen (G2+K1) XMM 73 (9) 27.1 2.2 -7.3, -6.2 Chandra 79 (1) Altair (A7) XMM 130 (1) 27.1 2.3 -7.4 data taken 1999-2007 , XMM/RGS binary data unresolved MOS/RGS spectral fit for basic parameter, LX in 0.2 – 3.0 keV band Jan Robrade (Hamburger Sternwarte) Ne/O in stellar coronae 26.07.2011 16 / 28
  • 17. Results - weakly active stars (Hempelmann 2006, Robrade+, in prep.) Global X-ray properties Pt. I all coronae are cool, av. TX ≈ 2 − 4 MK weak to minor contribution of 5 – 10 MK plasma FIP effect in the lesser active stars (α Cen, β Com) weak/no FIP effect in in moderately active stars many weakly active G and K dwarfs show cyclic X-ray activity Jan Robrade (Hamburger Sternwarte) Ne/O in stellar coronae 26.07.2011 17 / 28
  • 18. Results - Altair XMM-observation of Altair (Robrade & Schmitt, 2009) A7 star, Teff ≈ 7800 K, M = 1.8 M , Vsini ≈ 220 km/s, i ≈ 60◦ , X-ray source X-ray properties similar to inactive sun LX = 1.4 × 1027 erg/s, log LX /Lbol = −7.4, 1 – 4 MK plasma minor activity, rotational modulation, long term stable solar-like abundances and FIP effect ’classical interpretation’: thin outer convective layer Jan Robrade (Hamburger Sternwarte) Ne/O in stellar coronae 26.07.2011 18 / 28
  • 19. Results - Altair II Altair - rotationally deformed Vrot 60% breakup-speed ⇒ X-ray saturation level very low oblate, axial ratio of a / b ≈ 1.1 – 1.2 gravity darkening ⇒ Teff range: 6900 K (equator) up to 8500 K (poles) O vii f /i-ratio high: tracer of density and UV-field surface features at Teff 7400 K CHARA (Monnier et al. 2007) f /i = R0 /(1 + φ/φc + ne /nc ) (e.g. Gabriel & Jordan 1969, Porquet+ 2001) =⇒ Equatorial bulge corona Jan Robrade (Hamburger Sternwarte) Ne/O in stellar coronae 26.07.2011 19 / 28
  • 20. Neon and oxygen - results Global modeling - results Ne/O ratio robust Neon and oxygen line measurements virtually all lines detected in all stars few Ne x U.L. in LETGS spectra of coolest coronae account for Fe xvii blend in Ne x via emissivities (20 %) neglect Fe xix blends in Ne ix – low TX overall good agreement between multiple observations obs.-time average for cyclic stars Ne/O ratios - D&T vs. L&S similar for the hotter stars discrepancies for the coolest stars Jan Robrade (Hamburger Sternwarte) Ne/O in stellar coronae 26.07.2011 20 / 28
  • 21. Ne/O - results I Coronal stellar Ne/O ratios and the ’classical’ Sun (Robrade & Schmitt, 2009) (global fit: diamonds/solid line, D&T asterisks/dotted line, L&S squares/dashed line) Stellar X-ray data suggests Ne/O at upper bound of solar range Jan Robrade (Hamburger Sternwarte) Ne/O in stellar coronae 26.07.2011 21 / 28
  • 22. Ne/O - results II Ne/O ratios of individual stars Ne/O: 0.35 – 0.40 for Eri (0.37), 61 Cyg (0.36), HD 81809 (0.36) Ne/O: 0.25 – 0.35 for β Com (0.25), α Cen B (0.26) Ne/O: 0.20 – 0.25 for Procyon (0.22), α Cen A (0.21), Altair (0.20) overall good agreement with literature mod. active stars Eri (Wood & Linsky Ne/O = 0.36, Sanz-Forcada+ Ne/O = 0.4) weakly active stars Procyon (Raassen+ Ne/O = 0.22 , Sanz-Forcada+ Ne/O = 0.40) α Cen A/B (Raassen+ A: Ne/O = 0.18, B: Ne/O = 0.26, L&S Ne/O = 0.27) Jan Robrade (Hamburger Sternwarte) Ne/O in stellar coronae 26.07.2011 22 / 28
  • 23. Ne/O - results III Ne/O ratios of stellar coronae coronal Ne/O ratio increases with activity in weakly active stars trend independent of analysis method trend independent of spectral type Ne/O ≈ 0.2 at log LX /Lbol ≈ −6.5 Ne/O ≈ 0.4 at log LX /Lbol ≈ −4.5 solar values typical for low activity stars Ne/O apparently saturates at higher activity levels larger datasets required to reveal details of chemical fractionation shape of ratio-curve dependence on sp. type, LX /Lbol vs. TX Jan Robrade (Hamburger Sternwarte) Ne/O in stellar coronae 26.07.2011 23 / 28
  • 24. Solar modeling problem: further insights Other abundance determinations: low Ne/O ratio in photospheric study of early B stars (Przybilla et al. 2008) Ne/O= 0.21 (0.19-0.23) (absolute values intermediate to GS98 & AGS05) homogeneous distribution of elemental abundances in solar neighborhood Solar abundances revised (Asplund+ 2009) slightly higher solar metallicity (+ 10%) Ne/O = 0.17 (0.14-0.22) absolute abundances of Ne and O: agreement between Sun, B stars and H ii-regions within errors Lodders+ 2009, Ne/O = 0.21 Jan Robrade (Hamburger Sternwarte) Ne/O in stellar coronae 26.07.2011 24 / 28
  • 25. Caveats & open Questions Measured and predicted sound speed (Asplund+ 2009) Discrepancy to helioseismology alleviated but still significant! Solar problems sound speed profile wrong convection zone depth too shallow interior He abundance too low Possible solutions revise abundance calculations revise opacity calculations for solar interior revise diffusion model - interior is more metal rich internal gravity waves - promising, but only qualitatively evaluated Jan Robrade (Hamburger Sternwarte) Ne/O in stellar coronae 26.07.2011 25 / 28
  • 26. Caveats & open Questions II Chemical fractionation: cause of fractionation not fully explained transition: FIP- no-FIP - IFIP Laming-models promising (ponderomotive force) activity good tracer - importance of fundamental parameter elements: charge, mass stars: gravity, temperature gradients, radiation, electric & magnetic fields details of abundance trends need to be refined other elements need to be considered Jan Robrade (Hamburger Sternwarte) Ne/O in stellar coronae 26.07.2011 26 / 28
  • 27. Summary Neon and oxygen in stellar coronae Ne/O ratio depends on stellar activity Ne/O increases with activity in weakly to moderately active stars Ne/O ≈ 0.2 ± 0.05 in weakly active stars Neon is not the solution for the solar modelling problem The Sun is a typical star! Jan Robrade (Hamburger Sternwarte) Ne/O in stellar coronae 26.07.2011 27 / 28
  • 28. Ne/O - line fluxes Measured line fluxes in 10−5 photons cm−2 s−1 from RGS or LETGS (C) and energy flux ratio of the O viii(Lyα) to O vii(r) line. Star O vii(r) O viii Ne ix(r) Ne x∗ O8/O7(r) 61 Cyg 6.6±0.4 9.1±0.5 2.0±0.3 1.6±0.2 1.57±0.13 Altair 4.9±0.4 3.7±0.3 0.4±0.1 0.2±0.1 0.86±0.10 α Cen 33.5±1.3 27.0±1.2 4.1±0.5 1.6±0.2 0.92±0.05 α Cen 03/04 47.9±2.1 45.4±1.5 5.5±0.8 2.4±0.5 1.08±0.06 α Cen A (C) 9.2±1.0 3.2±0.5 0.5±0.3 0.2 0.40±0.07 α Cen B (C) 11.5±1.0 6.3±0.6 1.3±0.4 0.2 0.62±0.08 β Com 3.8±0.6 5.9±0.6 0.9±0.3 0.6±0.3 1.77±0.33 Eri 44.1±2.6 78.0±3.0 21.2±2.4 10.5±1.4 2.01±0.14 Eri (C) 41.5±1.6 78.9±1.7 18.8±0.9 16.7±0.9 2.16±0.10 HD 81809 1.0±0.3 2.3±0.3 0.5±0.2 0.5±0.2 2.62±0.86 Procyon 35.6±1.1 22.9±0.9 1.8±0.3 0.5±0.2 0.73±0.04 Procyon (C) 29.1±1.6 17.3±1.0 2.5±0.5 0.7±0.3 0.68±0.05 Procyon (C) 30.3±1.7 18.9±1.1 1.4±0.3 0.2 0.71±0.06 ∗ Blended with Fe xvii. Jan Robrade (Hamburger Sternwarte) Ne/O in stellar coronae 26.07.2011 28 / 28