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Table A.2:

Star-to-star (individual) errors and cluster errors in atmospheric parameters and in the EWs.
  Star-to-star errors   Cluster errors
cluster $T_{\rm eff}$ $\log g$ [A/H] vt EW   $T_{\rm eff}$ $\log g$ [A/H] vt
  (K) dex (dex) (km s-1) (dex)   (K) dex (dex) (km s-1)
  (1) (2) (3) (4) (5)   (6) (7) (8) (9)
NGC 104 6 0.042 0.032 0.11 0.025   40 0.059 0.026 0.009
NGC 288 6 0.041 0.042 0.28 0.025   63 0.061 0.070 0.027
NGC 1904 5 0.041 0.036 0.20 0.027   57 0.060 0.069 0.026
NGC 3201 4 0.041 0.049 0.19 0.028   62 0.061 0.073 0.016
NGC 4590 4 0.041 0.071 0.28 0.037   69 0.061 0.068 0.025
NGC 5904 12 0.041 0.023 0.11 0.024   54 0.060 0.062 0.009
NGC 6121 4 0.041 0.025 0.12 0.022   54 0.060 0.053 0.012
NGC 6171 2 0.041 0.044 0.21 0.025   26 0.057 0.026 0.037
NGC 6254 4 0.041 0.053 0.13 0.026   67 0.061 0.074 0.011
NGC 6388 9 0.043 0.078 0.19 0.037   57 0.061 0.028 0.032
NGC 6397 4 0.041 0.039 0.34 0.038   64 0.060 0.060 0.028
NGC 6808 5 0.041 0.044 0.20 0.027   58 0.060 0.072 0.016
NGC 6838 5 0.041 0.034 0.10 0.023   45 0.059 0.048 0.016
NGC 7078 5 0.041 0.061 0.33 0.030   67 0.061 0.067 0.036
NGC 7099 5 0.041 0.046 0.41 0.034   71 0.061 0.067 0.051
(1) Slope relation $T_{\rm eff}$(V-K) $_{\rm Alonso}$ vs. mag V or K + 0.02 mag error in V or K; (2) slope $\log g$ vs. mag V or K +0.02 mag error + 10% variation in mass; (3) rms scatter in [Fe/H] of all analysed stars; (4) quadratic mean of 1$\sigma $ errors in the slope abundances Fe I/line strength (minus systematic components) from stars with a large enough number of Fe I lines (5) (rms in Fe I for stars with enough lines) divided the square root of typical number of lines; (6) slope relation $T_{\rm eff}$(V-K) $_{\rm Alonso}$ vs. (V-K)0 +0.02 error in E(B-V) + 0.02 mag error in V-K colours zero point; (7) 0.1 mag error in modulus + systematic error in $T_{\rm eff}$ +10% error in mass; (8) statistical error+systematic error in $T_{\rm eff}$+systematic error in $\log g$ + systematic error in vt; (9) internal error in vt divided the square root of $N_{\rm stars}$.

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