VizieR

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VizieR

  
J/A+AS/147/111
  Iron Project. XLIV. Fe VI. (Chen+, 2000)
Post annotation
  
1.J/A+AS/147/111/table1The 80 fine structure levels corresponding to the 34 LS terms included in the calculations and their observed energies (Ry) in Fe VI (Sugar & Corliss, 1985, Cat. VI/74) (80 rows)
2.J/A+AS/147/111/table2Weighted dipole allowed E1 oscillator strengths gfL, gfV in the length and velocity formulations, and the Einstein A-coefficients AL in the length formulation. (867 rows)
3.J/A+AS/147/111/table3Comparison of the electric quadrupole (E2) and magnetic dipole (M1) transition probabilities between the first 19 levels of Fe VI in s–1 among the present calculation by SUPERSTRUCTURE, calculations by Garstang et al. (1978ApJ...222..384G) and by Nussba (129 rows)
4.J/A+AS/147/111/table4Electric quadrupole (E2) and magnetic dipole (M1) transition probabilities between the first 80 levels of Fe VI in s–1 in the present calculation by SUPERSTRUCTURE. (1101 rows)
5.J/A+AS/147/111/table6Line intensity ratios for transitions relative to λ5146Å (8-3: 4F7/2-2G7/2), with Teff=150000K. (177 rows)

 
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Column  Constraint Explain   (UCD)
  (ALL)recno  Record number assigned by the VizieR team. Should Not be used for identification. (meta.record)
   (ALL)i  Initial level (meta.id)
  (1)Term (char) LS term (phys.atmol.configuration)
  (1)2J  Final 2J level (phys.atmol.qn)
  (1)E Ry Observed energy (Sugar & Corliss, 1985, Cat. VI/74) (phys.energy;phys.atmol.level)
  (2+3+4+5)j  Final level (meta.id)
  (2)gfL  E1 oscillator strength in the length formulation (phys.atmol.wOscStrength)
  (2)gfV  E1 oscillator strength in the velocity formulation (phys.atmol.wOscStrength)
  (2)AL s-1 Einstein A-coefficient in the length formulation (phys.atmol.transProb)
  (3+4)E2 s-1 Present electric quadrupole transition probability (phys.atmol.transProb)
  (3+4)M1 s-1 Present magnetic dipole transition probability (phys.atmol.transProb)

ALL cols
    
 (i)indexed column
  (3)E2G s-1 (n) Garstang et al. (1978ApJ...222..384G) electric quadrupole transition probability (phys.atmol.transProb)
  (3)M1G s-1 (n) Garstang et al. (1978ApJ...222..384G) magnetic dipole transition probability (phys.atmol.transProb)
  (3)E2N s-1 (n) Nussbaumer & Storey (1978A&A....70...37N) electric quadrupole transition probability (phys.atmol.transProb)
  (3)M1N s-1 (n) Nussbaumer & Storey (1978A&A....70...37N) magnetic dipole transition probability (phys.atmol.transProb)
  (5)lambda nm Wavelength (em.wl;phys.atmol.transition)
  (5)FLE (char) [ABCDEO] Note on fluorescent excitation (Note 1)   (meta.code)
  (5)LIR1  (n) Te=10000K, ne=103cm-3 line intensity ratio (spect.line.intensity;arith.ratio)
  (5)LIR2  (n) Te=10000K, ne=104cm-3 line intensity ratio (spect.line.intensity;arith.ratio)
  (5)LIR3  (n) Te=20000K, ne=103cm-3 line intensity ratio (spect.line.intensity;arith.ratio)
  (5)LIR4  (n) Te=20000K, ne=104cm-3 line intensity ratio (spect.line.intensity;arith.ratio)
  (5)LIR5  (n) Te=12000K, ne=2x103cm-3 line intensity ratio (spect.line.intensity;arith.ratio)
  (5)LIR6  (n) Te=12000K, ne=6x103cm-3 line intensity ratio (spect.line.intensity;arith.ratio)
  (5)LIR7  (n) Te=12000K, ne=104cm-3 line intensity ratio (spect.line.intensity;arith.ratio)

ALL cols
    
(n) indicates a possible blank or NULL column(i)indexed column
  (5)LIR8  (n) Te=16000K, ne=2x103cm-3 line intensity ratio (spect.line.intensity;arith.ratio)
  (5)LIR9  (n) Te=16000K, ne=6x103cm-3 line intensity ratio (spect.line.intensity;arith.ratio)
  (5)LIR10  (n) Te=16000K, ne=104cm-3 line intensity ratio (spect.line.intensity;arith.ratio)
  (5)LIR11  (n) Line intensity ratio from r_LIR11 (spect.line.intensity;arith.ratio)
  (5)r_LIR11 (char) [a-f] Reference for LIR11 (Note 2)   (meta.ref)

ALL cols
    
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