J/AJ/106/1059       Lithium in the Pleiades      (Soderblom+, 1993)
The evolution of the lithium abundances of solar-type stars. III. The Pleiades
     Soderblom D.R., Jones B.F., Balachandran S., Stauffer J.R.,
     Duncan D.K., Fedele S.B., Hudon J.D.
    <Astron. J. 106, 1059 (1993)>
    =1993AJ....106.1059S 1993AJ....106.1059S      (SIMBAD/NED Reference)
ADC_Keywords: Abundances ; Clusters, open
Abstract:
    We report new measurements of lithium in more than 100 Pleiades F, G,
    and K dwarfs. Abundances were determined from spectrum synthesis fits
    to the data as well as from use of new curves of growth for the
    Li 6708 A feature (presented in an Appendix). We confirm the intrinsic
    spread in lithium abundance within the Pleiades seen by Duncan & Jones
    (1983ApJ...271..663D 1983ApJ...271..663D), but we establish more observational constraints
    on Li in this cluster: First, for stars near 1.0Msun [about 0.60 to
    0.75 in (B-V)0], the scatter in the relation between log N(Li) (defined
    as N(Li)) and T(eff) is consistent with our observational uncertainty.
    That means that most late-F and early-G dwarfs in the Pleiades are
    consistent with the tight N(Li) versus mass relation seen in the Hyades
    in the same mass range. Second, at (B-V)0∼0.8 (M∼0.9Msun), large and
    real star-to-star differences in N(Li) appear. The range in N(Li) at
    (B-V)0∼0.8 is about 1dex, and grows to as much as 1.5dex for less massive
    stars. Third, the most Li-rich stars have abundances at or near the
    primordial level for Population I (N(Li)∼3.2), and none exceed that
    level by a significant amount. Fourth, at any given color the stars that
    rotate fastest have the most Li and have the strongest chromospheric
    activity. We consider the ways in which an apparent spread in N(Li)
    could arise from an intrinsically tight N(Li)-mass relation and conclude
    that the spread is probably real and is not an artifact of line formation
    conditions or inhomogeneous atmospheres on the stars. It is possible to
    produce large apparent changes in N(Li) by covering a significant fraction
    of a star's surface with cooler regions ("spots"), but doing so has other
    ramifications that conflict with the observations. Some current models lead
    to a spread in N(Li) in which the fastest rotators (those that have lost
    the least angular momentum) have the most Li, and that mechanism may
    account for what is seen. A comparison of the Pleiades to the Alpha
    Persei cluster shows that most Alpha Persei stars have Li abundances
    comparable to their Pleiades counterparts, but there is a significant
    fraction (about 30%) of Alpha Persei stars that lie below the Pleiades
    in N(Li) by 1dex or more. Some of these anomalous stars have even
    less Li than Hyades stars of the same T(eff). If these stars are bona
    fide Alpha Persei members (and they probably are), their Li abundances
    strain our understanding of Li depletion. The Pleiades, considered
    together with Alpha Persei and the Hyades, shows that stars with
    [Fe/H]≥0.0 and which are more massive than about 1.25Msun do not
    deplete Li prior to reaching main the sequence. Moreover, solar-abundance
    stars ([Fe/H]∼0.0) with M≳1.1Msun do not experience pre-main-sequence
    depletion either. Pleiades dwarfs near T(eff)=6700K show evidence of being
    depleted in Li, indicating that an incipient Li "chasm" is present even at
    an age of 70Myr.
File Summary:
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 File Name   Lrecl    Records    Explanations
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ReadMe          80          .    This file
table1          79         131   Observations of Lithium in Pleiades F, G,
                                  and K dwarfs
table2          85          61  *Lithium abundances for the 6708 A feature
table3          85          51  *Lithium abundances for the 6104 A feature
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Note on table2, table3:  A grid of curves of growth was computed for every
    250K in T(eff) from 4000 to 6500K, and for every 0.2dex in logN(Li).
    A microturbulent velocity of 1.0km/s was used for the tables given
    here, but computations for Xi=2km/s differ little. One dimensional
    interpolation was done to create points evenly spaced in log W(lambda)
    with log N(Li) as the dependent variable.
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Byte-by-byte Description of file: table1
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   Bytes Format  Units   Label    Explanations
--------------------------------------------------------------------------------
   1-  4  A4     ---     fgk      fgk number from Soderblom et al.
                                   (1993ApJS...85..315S 1993ApJS...85..315S) (hereafter SSHJ)
   6-  9  A4     ---     name     Hertzsprung (H II) designation.
                                   A "P" prefix denotes a Pels star.
  11- 16  A6     ---     Sp       Spectral type
  17- 21  F5.3   mag     (B-V)0   Dereddened (B-V)
      22  A1     ---   u_(B-V)0   Uncertainty flag on (B-V)0
  24- 27  I4     K       Teff     Effective temperature
      29  A1     ---   l_vsini    Limit flag on vsini
  30- 34  F5.1   km/s    vsini    ? Rotational velocity
      35  A1     ---   u_vsini    uncertainty flag on vsini
      36  A1     ---   n_vsini    [S ] 'S' indicating a double-lined
                                   spectroscopic binary whose vsini values are
                                   given in table2 of SSHJ (SB2).
  38- 42  F5.2   --- log(RHalpha) []? Ratio of the Halpha flux to the stellar
                                   bolometric flux, log R(Halpha) from SSHJ
  44- 48  F5.2   --- log(R8542)   []? Ratio of the 8542 A Ca II line flux to the
                                   stellar bolometric flux, logR(8542) from SSHJ
  51- 53  I3     0.1pm   W7699    []? Equivalent width of K I 7699A line
  56- 58  I3     0.1pm   W6717    []? Equivalent width of Ca I 6717 A line
      59  A1     ---   n_W6717    Note on W6717. See note (1)
      60  A1     ---   l_W6708    Limit flag on W6708
  61- 63  I3     0.1pm   W6708    Equivalent width of Li I 6708 A line,
                                   corrected for Fe I 6707.441.
      64  A1     ---   u_W6708    Uncertainty flag on W6708
      65  A1     ---   n_W6708    Note on W6708. See note (1)
  67- 72  A6     ---     q        Source and quality code (2)
      73  A1     --- l_log(N(Li)) Limiting character for lithium abundance
  75- 78  F4.2   ---   log(N(Li)) Abundance of lithium (scale logN(H)=12)
      79  A1     --- u_log(N(Li)) Uncertainty flag on log(N(Li))
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Note (1): A '*' indicates that equivalent width of the line has been
    compensated for spectrum dilution by the following factors:
    H II 102, 1.33; H II 173, 1.40; H II 248 and 2147, 1.20;
    H II 298, 571, 1100, and 2406, 1.10; H II 320, 1.15; H II 1101, 1.25.
Note (2): Source and quality code:
    Bo = Boesgaard et al. 1988b,  =1988ApJ...327..389B 1988ApJ...327..389B
    Bu = Butler et al. 1987,      =1987ApJ...319L..19B 1987ApJ...319L..19B
    P  = Pilachowski et al. 1987, =1987PASP...99.1288P 1987PASP...99.1288P
    Codes a to d denote Lick data and are in descending order of quality,
    with approximate uncertainties of 12, 18, 25, and 40 mA, respectively
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Byte-by-byte Description of file: table2 table3
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   Bytes Format  Units   Label    Explanations
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   4-  7  F4.2 [0.1pm] log(W6708) Equivalent width of Li 6708 line
  10- 15  F6.3   ---   logN(Li)1  Li abundance for Teff = 4000 K
  17- 22  F6.3   ---   logN(Li)2  Li abundance for Teff = 4250 K
  24- 29  F6.3   ---   logN(Li)3  Li abundance for Teff = 4500 K
  31- 36  F6.3   ---   logN(Li)4  []? Li abundance for Teff = 4750 K
  38- 43  F6.3   ---   logN(Li)5  []? Li abundance for Teff = 5000 K
  45- 50  F6.3   ---   logN(Li)6  []? Li abundance for Teff = 5250 K
  52- 57  F6.3   ---   logN(Li)7  []? Li abundance for Teff = 5500 K
  59- 64  F6.3   ---   logN(Li)8  []? Li abundance for Teff = 5750 K
  66- 71  F6.3   ---   logN(Li)9  []? Li abundance for Teff = 6000 K
  73- 78  F6.3   ---   logN(Li)10 []? Li abundance for Teff = 6250 K
  80- 85  F6.3   ---   logN(Li)11 []? Li abundance for Teff = 6500 K
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Origin: AAS CD-ROM series, Volume 1, 1993
(End)                                         Patricia Bauer [CDS]   12-Sep-1994