VizieR

CfA VizieR . ADAC VizieR . Cambridge (UK) VizieR . IUCAA VizieR . INASAN VizieR .

VizieR

  
J/ApJS/182/51
  Transition probabilities of rare earth elements (Lawler+, 2009)
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1.J/ApJS/182/51/table2Atomic transition probabilities for CeII (Z=58) organized by increasing wavelength in air (921 rows)
2.J/ApJS/182/51/table5Experimental atomic transition probabilities for LaII (Z=57) arranged by Wavenumber from Lawler et al. (2001ApJ...556..452L) (84 rows)
3.J/ApJS/182/51/table6Experimental atomic transition probabilities for EuII (Z=63) arranged by wavenumber from Lawler et al. (2001ApJ...563.1075L) (24 rows)
4.J/ApJS/182/51/table7Hyperfine structure line component patterns for 159TbII (Z=65). (1735 rows)
5.J/ApJS/182/51/table8Experimental atomic transition probabilities for DyI (Z=66; levels have integral J) and DyII (levels have half integral J) from Wickliffe et al. (2000JQSRT..66..363W) (915 rows)
6.J/ApJS/182/51/table9Experimental atomic transition probabilities for HoII (Z=67) arranged by Wavenumber from Lawler et al. (2004ApJ...604..850L) (22 rows)
7.J/ApJS/182/51/table10Hyperfine structure line component patterns for HoII (Z=67). (473 rows)
8.J/ApJS/182/51/table11Experimental atomic transition probabilities for TmII (Z=69) from Wickliffe & Lawler (1997JOSAB..14..737W) (146 rows)
9.J/ApJS/182/51/table13*Experimental atomic transition probabilities for LuII (Z=71) from odd-parity upper levels organized by increasing wavelength in air. (Note) (19 rows)
10.J/ApJS/182/51/table14Hyperfine structure line component patterns for 175LuII (Z=71). (163 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)lamAir 0.1nm Wavelength in air in Angstroms (em.wl;phys.atmol.transition)
  (1+2+3+5+6+8+9)E1 cm-1 Upper level energy (phys.energy;phys.atmol.level)
  (1+5+8)p1 (char) Upper level parity (phys.atmol.parity;phys.atmol.level)
  (1+2+3+5+6+8+9)J1  Upper level J value (phys.angMomentum;phys.atmol.level)
  (1+2+3+5+6+8+9)E0 cm-1 Lower level energy (phys.energy;phys.atmol.level)
  (1+5+8)p0 (char) Lower level parity (phys.atmol.parity;phys.atmol.level)
  (1+2+3+5+6+8+9)J0  Lower level J value (phys.angMomentum;phys.atmol.level)
  (1+2+3+6+8+9)Aij 10+6/s Transition probability (phys.atmol.transProb)
  (1+2+3+6+9)e_Aij 10+6/s Total uncertainty in Aij (stat.error;phys.atmol.transProb)
  (1)log(gf)  Log of degeneracy times oscillator strength (phys.atmol.oscStrength)

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 (i)indexed column
  (2+3+4+5+6+7+8+10)sigma cm-1 (n) Transition Wavenumber (except for table13) (phys.energy;phys.atmol.transition)
  (2+3+6+8+9)log(gf) [-] Log of degeneracy times oscillator strength (phys.atmol.oscStrength)
  (4+7+10)F1  Component upper level F or total angular momentum (phys.atmol.qn)
  (4+7+10)F0  Component lower level F or total angular momentum (phys.atmol.qn)
  (4+7+10)dsigma cm-1 Component offset Wavenumber with respect to Center-of-gravity Wavenumber (stat.fit.omc;phys.energy)
  (4+7+10)dlam 0.1nm Component offset Wavelength with respect to Center-of-gravity Wavelength (em.wl;arith.diff)
  (4+7+10)Strength  Component strength (Note 1)   (spect.line.width)
  (5)AijW 10+6/s (n) Transition probability from Univ. Wisconsin (phys.atmol.transProb)
  (5)e_AijW % (n) Percent total uncertainty in AijW (stat.error)
  (5)log(gf)W [-] (n) Log of degeneracy times oscillator strength from Univ. Wisconsin (phys.atmol.oscStrength)
  (5)AijN 10+6/s (n) Transition probability from NIST (phys.atmol.transProb)
  (5)e_AijN % (n) Percent total uncertainty in AijN (stat.error)
  (5)log(gf)N [-] (n) Log of degeneracy times oscillator strength from NIST (phys.atmol.oscStrength)

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(n) indicates a possible blank or NULL column(i)indexed column
  (6)log(gf)O [-] (n) Log of degeneracy times oscillator strength, from another source (phys.atmol.oscStrength)
  (6)r_log(gf)O (char) Note on log(gf)O (Note 1)   (meta.ref;pos.frame)
  (8)e_Aij % Percent total uncertainty in Aij (stat.error;phys.atmol.transProb)

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(n) indicates a possible blank or NULL column(i)indexed column
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