J/A+AS/130/541 Co II oscillator strengths (Raassen+ 1998)
Calculated oscillator strengths of singly ionized Cobalt
Raassen A.J.J., Pickering J.C., Uylings P.H.M.
<Astron. Astrophys. Suppl. Ser. 130, 541 (1998)>
=1998A&AS..130..541R 1998A&AS..130..541R (SIMBAD/NED BibCode)
ADC_Keywords: Atomic physics
Keywords: atomic data - ISM: abundances - stars: chemically peculiar -
supernovae
Description:
In table 2 the log(gf) values for the 3d8+3d7 4s-->3d7 4p
electric dipole (E1) transitions are given. This system is selected by
cutting off energy values larger than 120,000cm-1 of both the even
and the odd system in the final printing procedure; only log(gf)
values larger than -3 are included. The first column of this table
shows the wavelength obtained from the energy differences between the
experimental level values. Wavelengths below 2000 Angstrom are given
as vacuum wavelengths and above 2000 Angstrom as air wavelengths. The
second column gives the log(gf) values followed by the J-value, energy
value and the name of the lower (even) level. The first character of
the level name designates the configuration number: for the even
levels '1' refers to 3d8 and '2' to 3d7 4s; for the odd levels '1'
refers to 3d7 4p. An '*' after the energy value indicates that the
level is known, in which case the experimental level value is given.
When unknown, the calculated energy value is given and used to
approximate the wavelength.
The A-values for the forbidden lines given in table 7 are restricted
to the magnetic dipole (M1) and electric quadrupole (E2) transitions
within the 3d8+3d7 4s configurations, from levels with an energy
of less than 50,000 cm-1 above the ground and with A-values larger
than 10-3s-1. The level with the lower J-value is given first in
the designation of the transition. The remaining columns are similar
to the corresponding ones in table 2. The first character of the level
name designates the configuration number: for the even levels '1'
refers to 3d^8 and '2' to 3d^7 4s. An '*' after the energy value
indicates that the level is known, in which case the experimental
level value is given. When unknown, the calculated energy value is
given and used to approximate the wavelength.
File Summary:
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FileName Lrecl Records Explanations
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ReadMe 80 . See above
table2.dat 80 12168 log(gf) values for the 3d8+3d7 4s-->3d7 4p
electric dipole (E1) transitions
table7.dat 109 434 A-values for the forbidden lines
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See also:
J/A+A/389/716 : Oscillator strengths for Li-like ions (Nahar, 2002)
Byte-by-byte Description of file: table2.dat
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Bytes Format Units Label Explanations
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2- 12 F11.3 0.1nm lambda Wavelength
14- 24 F11.5 --- loggf log(gf) value
26- 29 F4.1 --- Jf J-value final state
31- 40 F10.2 cm-1 Ef Energy value final state
41 A1 --- n_Ef [*] Indication known/unknown
43- 52 A10 --- Lf Leading term final state
54- 57 F4.1 --- Ji J-value initial state
59- 68 F10.2 cm-1 Ei Energy value initial state
69 A1 --- n_Ei [*] Indication known/unknown
71- 80 A10 --- Li Leading term initial state
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Byte-by-byte Description of file: table7.dat
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Bytes Format Units Label Explanations
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2- 12 F11.3 0.1nm lambda Wavelength
14- 20 E7.2 s-1 A(M1) ? A-value (M1)
24- 30 E7.2 s-1 A(E2) ? A-value (E2)
34- 37 F4.1 --- Jf J-value final state
39- 48 F10.2 cm-1 Ef Energy value final state
49 A1 --- n_Ef [*] Indication known/unknown
51- 60 A10 --- Lf Leading term final state
62- 65 F4.1 --- Ji J-value initial state
67- 76 F10.2 cm-1 Ei Energy value initial state
77 A1 --- n_Ei [*] Indication known/unknown
79- 88 A10 --- Li Leading term initial state
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Acknowledgements: P. Uylings
(End) Patricia Bauer [CDS] 23-Jan-1998