O + 3 8 4 624383.8(1S) 706796.6(3P) 1 2S2 2P (2)1( 2.5) 0. {1}1.500 {2}1.500 2 2S1 2P2 (4)1( 5.5) 71641. {2}3.000 3 2S1 2P2 (2)2( 4.5) 126942. {1}0.500 {2}1.500 4 2S1 2P2 (2)0( 0.5) 164366. {1}0.500 {2}1.500 5 2S1 2P2 (2)1( 2.5) 180642. {1}0.500 {2}1.500 6 2P3 (4)0( 1.5) 231537. {X} 7 2P3 (2)2( 4.5) 255167. {X} 8 2P3 (2)1( 2.5) 289022. {X} -1 4.00 3 1.60+04 3.20+04 8.00+04 1.60+05 3.20+05 8.00+05 1.60+06 3.20+06 2 1 1.00-30 1.41+00 1.55+00 1.46+00 1.24+00 1.08+00 8.91-01 7.07-01 5.14-01 3 1 7.09+08 6.88+00 6.84+00 6.41+00 6.24+00 6.31+00 6.55+00 6.86+00 7.35+00 4 1 3.84+09 1.96+00 1.89+00 1.88+00 1.97+00 2.10+00 2.31+00 2.58+00 2.94+00 5 1 7.44+09 7.42+00 7.54+00 7.88+00 8.43+00 9.14+00 1.04+01 1.19+01 1.39+01 6 1 1.00-30 1.09-02 1.07-02 9.69-03 8.52-03 7.18-03 5.02-03 3.46-03 2.20-03 7 1 1.00-30 3.85-01 3.79-01 3.63-01 3.47-01 3.36-01 3.36-01 3.36-01 3.36-01 8 1 1.00-30 2.09-01 2.08-01 2.06-01 2.01-01 1.96-01 1.96-01 1.96-01 1.96-01 3 2 1.00-30 3.50+00 3.47+00 3.20+00 2.84+00 2.40+00 1.72+00 1.20+00 7.74-01 4 2 1.00-30 4.42-01 4.09-01 3.64-01 3.22-01 2.61-01 1.68-01 1.09-01 6.56-02 5 2 1.00-30 1.46+00 1.39+00 1.12+00 8.47-01 6.05-01 3.45-01 2.07-01 1.17-01 6 2 6.55+09 6.94+00 7.07+00 7.41+00 7.99+00 8.66+00 9.75+00 1.10+01 1.28+01 7 2 1.00-30 8.12-01 7.95-01 7.50-01 6.96-01 6.12-01 4.59-01 3.34-01 2.23-01 8 2 1.00-30 2.88-01 2.85-01 2.73-01 2.54-01 2.26-01 1.75-01 1.31-01 8.93-02 4 3 1.00-30 6.67-01 6.69-01 6.76-01 6.88-01 7.14-01 7.84-01 8.60-01 9.46-01 5 3 1.00-30 1.53+00 1.51+00 1.44+00 1.32+00 1.14+00 8.21-01 5.82-01 3.65-01 5 4 1.00-30 2.42-01 2.39-01 2.29-01 2.10-01 1.80-01 1.30-01 9.21-02 5.82-02 R 1 +1 3.67-12 2.64-12 1.50-12 9.00-13 5.22-13 2.48-13 1.44-13 7.28-14 R 2 +1 1.00-30 1.00-30 1.00-30 1.00-30 1.00-30 1.00-30 1.00-30 1.00-30 R 3 +1 1.01-11 5.19-12 2.21-12 1.05-12 4.49-13 1.29-13 4.78-14 1.73-14 R 4 +1 6.08-13 5.62-13 3.78-13 2.07-13 9.38-14 2.78-14 1.04-14 3.78-15 R 5 +1 2.55-13 3.42-13 3.01-13 1.87-13 9.11-14 2.84-14 1.08-14 3.96-15 R 6 +1 1.00-30 1.00-30 1.00-30 1.00-30 1.00-30 1.00-30 1.00-30 1.00-30 R 7 +1 1.81-12 1.85-12 8.97-13 4.01-13 1.61-13 4.42-14 1.61-14 5.77-15 R 8 +1 1.04-12 1.18-12 6.44-13 3.04-13 1.26-13 3.53-14 1.29-14 4.65-15 R 1 +2 4.11-13 2.71-13 1.57-13 1.01-13 6.42-14 4.05-14 2.23-14 1.45-14 R 2 +2 1.69-12 1.07-12 5.80-13 3.58-13 2.15-13 1.08-13 6.36-14 3.24-14 R 3 +2 7.18-13 5.08-13 2.96-13 1.84-13 1.13-13 5.36-14 3.13-14 1.57-14 R 4 +2 9.51-14 6.60-14 3.98-14 2.64-14 1.72-14 8.26-15 4.72-15 2.44-15 R 5 +2 7.35-13 4.49-13 2.22-13 1.24-13 6.85-14 2.84-14 1.49-14 7.50-15 R 6 +2 3.64-13 3.44-13 1.98-13 1.04-13 4.65-14 1.37-14 5.12-15 1.86-15 R 7 +2 3.44-13 4.17-13 2.86-13 1.54-13 6.89-14 2.03-14 7.54-15 2.74-15 R 8 +2 1.23-12 6.78-13 2.65-13 1.18-13 4.81-14 1.34-14 4.92-15 1.77-15 -1 -1 -1 C---------------------------------------------------------------------------- C C Energy levels C Taken from Edlen (Phys Scr 28, 483, 1983) which are at most 14 cm-1 C in 126950 cm-1 different from those of NSRDS NBS 3 Sect 10. C C Ionisation Potential C Taken from Kelly (J Phys Chem Ref Data 16, 1987). C C A values C Compared by Hayes (J Phys B 16, 285, 1983) who points out that the values C of Seraph (J Phys B 13, 3129, 1980) are very accurate. The results of C Seraph were used. The length result of Hayes are < 10% different from Seraph C and C have length and velocity agreement of the order of 10%, apart from two C transitions. Dankwort and Treffetz (Ast and Ast 65, 93, 1978) have results C in good agreement with Hayes ( 5%), both using the same set of C configurations. C C Collision Data C The results of Hayes (1983) are used for transitions from 2s22p 2P and C 2s2p2 4P. These are from a close coupling calculation, for energies from C threshold to 5.6 Rydbergs. Resonance structure obtained in reactance C matrices and the resulting analytical fits are used to generate collision C strengths at a fine energy mesh. The wavefunctions were from Superstructure C and the close coupling calculation by Colalg and Impact. Care was taken to C get enough partial waves and to solve the problem of pseudoresonances. C A major improvement was the inclusion of closed channel resonances, C increasing intercombination rates by 40% in one case and a factor 2 in C another. C For 3-4, 3-5 and 4-5 transitions the 5 state close coupling results of C Robb (taken from Merts et al LA 8267 MS, 1980) were used. These do not C include closed channel resonances. C C C J Lang February 1990 C---------------------------------------------------------------------------- C C Radiative recombination data added - processed by adasrrc on C JETSHP.RADREC.BELIKE(O4LS) C C H P Summers Aug 1992. C C C---------------------------------------------------------------------------- C C Dielectronic data is post-processed from Badnell files as follows: C C /JETSHP.BADNELL.BELIKE(O4LS22) C /JETSHP.BADNELL.BELIKE(O4LS23) C C The cross-referencing file is as follows: C C /JETSHP.BADNELL.XREFDAT(O3L) C C The parent metastable indices are as follows: C C 1. 2S2 (1)0( 0.0) C 2. 2S1 2P1 (3)1( 4.0) C C Dielectronic data added to 6 existing rad. recom. level sets C C 18/08/92 C------------------------------------------------------------------------------- C C Update: C Fixed formatting on first line of file C Allan Whiteford, 28/07/08 C C------------------------------------------------------------------------------- C--------------------------------------------------------------------------------- C ADAS ADF04 DATA - SCCS info: @(#)$Header: /home/adascvs/adas/adf04/blike/blike_jl1989o.dat,v 2.2 2008/07/28 11:19:39 allan Exp $ Date $Date: 2008/07/28 11:19:39 $ C--------------------------------------------------------------------------------- C----------------------------------------------------------------------- C OPEN-ADAS C +++++++++ C C This file has been downloaded from OPEN-ADAS (http://open.adas.ac.uk) C on 28-Mar-2024. C C TERMS AND CONDITIONS C -------------------- C C The user of the OPEN-ADAS system and data (hereinafter "the User") C accepts the following terms and conditions: C C 1. The University of Strathclyde uses all reasonable endeavours to C ensure the accuracy of the data provided and any information C given, but the University makes no warranty, expressed or implied C as to its accuracy, integrity, fitness for purpose and shall not C be responsible for the use to which the data is put by the User C and/or any consequences arising out of any inaccuracies or C omissions. C C 2. Any downloaded OPEN-ADAS file is made available for the C personal use of the User only. It must not be used for any C commercial application, incorporated into any web site or in C any form re-distributed without express prior written permission C from the ADAS Project. In particular, but not by way of C limitation, it must not be: C * inserted into a managed database structure, C * redistributed along with a modelling or analysis code, C * made available on a public website. C C Permission for OPEN-ADAS data incorporation in non-commercial C code/system development for scientific advance will not be C unreasonably withheld, but will be subject to written agreement C on a case by case basis. C C The User will indemnify the University of Strathclyde and keep it C fully and effectively indemnified against each and every claim made C against the University as a result of the User's use of the data. C C-----------------------------------------------------------------------