Sample of transition data provided electronically at Zenodo. λobs and λcalc are the observed (if available, otherwise zero) and theoretical wavelengths (in Å) of the transition, respectively; fL and fV are the absorption oscillator strengths in the length and velocity forms, respectively; Aul is the transition rate (in s−1); Iup is the ionization energy (in Rydbergs) of the upper level to the respective parent; and ϵul is the emissivity (in erg s−1), as defined in Section 4, using an electron temperature of 7000 K and electron density of 6 × 1010 cm−3.
| λobs . | λcalc . | fL . | fV . | Aul . | Lower level . | Upper level . | Iup . | ϵul . |
|---|---|---|---|---|---|---|---|---|
| 0.00 | 1102.557 | 9.358(−5) | 8.937(−5) | 1.712(+5) | 2s2 2p23P0 | 2s2 2p(2P|$_{1/2}^{\rm o}$|) 30d 2[3/2]|$^o_1$| | 1.11253(−3) | 3.355(−17) |
| 0.00 | 1102.558 | 5.455(−6) | 5.345(−6) | 9.977(+3) | 2s2 2p23P0 | 2s2 2p(2P|$_{1/2}^{\rm o}$|) 31s 2[1/2]|$^o_1$| | 1.11343(−3) | 1.955(−18) |
| 0.00 | 1102.617 | 2.550(−5) | 2.430(−5) | 4.663(+4) | 2s2 2p23P0 | 2s2 2p(2P|$_{3/2}^{\rm o}$|) 24d 2[1/2]|$^o_1$| | 1.73510(−3) | 9.266(−18) |
| 0.00 | 1102.618 | 6.034(−5) | 5.792(−5) | 1.103(+5) | 2s2 2p23P0 | 2s2 2p(2P|$_{3/2}^{\rm o}$|) 24d 2[3/2]|$^o_1$| | 1.73617(−3) | 2.192(−17) |
| 0.00 | 1102.626 | 8.681(−6) | 8.180(−6) | 1.588(+4) | 2s2 2p23P0 | 2s2 2p(2P|$_{3/2}^{\rm o}$|) 25s 2[3/2]|$^o_1$| | 1.74176(−3) | 3.156(−18) |
| 0.00 | 1102.662 | 1.104(−4) | 1.054(−4) | 2.019(+5) | 2s2 2p23P0 | 2s2 2p(2P|$_{1/2}^{\rm o}$|) 29d 2[3/2]|$^o_1$| | 1.19101(−3) | 3.963(−17) |
| λobs . | λcalc . | fL . | fV . | Aul . | Lower level . | Upper level . | Iup . | ϵul . |
|---|---|---|---|---|---|---|---|---|
| 0.00 | 1102.557 | 9.358(−5) | 8.937(−5) | 1.712(+5) | 2s2 2p23P0 | 2s2 2p(2P|$_{1/2}^{\rm o}$|) 30d 2[3/2]|$^o_1$| | 1.11253(−3) | 3.355(−17) |
| 0.00 | 1102.558 | 5.455(−6) | 5.345(−6) | 9.977(+3) | 2s2 2p23P0 | 2s2 2p(2P|$_{1/2}^{\rm o}$|) 31s 2[1/2]|$^o_1$| | 1.11343(−3) | 1.955(−18) |
| 0.00 | 1102.617 | 2.550(−5) | 2.430(−5) | 4.663(+4) | 2s2 2p23P0 | 2s2 2p(2P|$_{3/2}^{\rm o}$|) 24d 2[1/2]|$^o_1$| | 1.73510(−3) | 9.266(−18) |
| 0.00 | 1102.618 | 6.034(−5) | 5.792(−5) | 1.103(+5) | 2s2 2p23P0 | 2s2 2p(2P|$_{3/2}^{\rm o}$|) 24d 2[3/2]|$^o_1$| | 1.73617(−3) | 2.192(−17) |
| 0.00 | 1102.626 | 8.681(−6) | 8.180(−6) | 1.588(+4) | 2s2 2p23P0 | 2s2 2p(2P|$_{3/2}^{\rm o}$|) 25s 2[3/2]|$^o_1$| | 1.74176(−3) | 3.156(−18) |
| 0.00 | 1102.662 | 1.104(−4) | 1.054(−4) | 2.019(+5) | 2s2 2p23P0 | 2s2 2p(2P|$_{1/2}^{\rm o}$|) 29d 2[3/2]|$^o_1$| | 1.19101(−3) | 3.963(−17) |
Sample of transition data provided electronically at Zenodo. λobs and λcalc are the observed (if available, otherwise zero) and theoretical wavelengths (in Å) of the transition, respectively; fL and fV are the absorption oscillator strengths in the length and velocity forms, respectively; Aul is the transition rate (in s−1); Iup is the ionization energy (in Rydbergs) of the upper level to the respective parent; and ϵul is the emissivity (in erg s−1), as defined in Section 4, using an electron temperature of 7000 K and electron density of 6 × 1010 cm−3.
| λobs . | λcalc . | fL . | fV . | Aul . | Lower level . | Upper level . | Iup . | ϵul . |
|---|---|---|---|---|---|---|---|---|
| 0.00 | 1102.557 | 9.358(−5) | 8.937(−5) | 1.712(+5) | 2s2 2p23P0 | 2s2 2p(2P|$_{1/2}^{\rm o}$|) 30d 2[3/2]|$^o_1$| | 1.11253(−3) | 3.355(−17) |
| 0.00 | 1102.558 | 5.455(−6) | 5.345(−6) | 9.977(+3) | 2s2 2p23P0 | 2s2 2p(2P|$_{1/2}^{\rm o}$|) 31s 2[1/2]|$^o_1$| | 1.11343(−3) | 1.955(−18) |
| 0.00 | 1102.617 | 2.550(−5) | 2.430(−5) | 4.663(+4) | 2s2 2p23P0 | 2s2 2p(2P|$_{3/2}^{\rm o}$|) 24d 2[1/2]|$^o_1$| | 1.73510(−3) | 9.266(−18) |
| 0.00 | 1102.618 | 6.034(−5) | 5.792(−5) | 1.103(+5) | 2s2 2p23P0 | 2s2 2p(2P|$_{3/2}^{\rm o}$|) 24d 2[3/2]|$^o_1$| | 1.73617(−3) | 2.192(−17) |
| 0.00 | 1102.626 | 8.681(−6) | 8.180(−6) | 1.588(+4) | 2s2 2p23P0 | 2s2 2p(2P|$_{3/2}^{\rm o}$|) 25s 2[3/2]|$^o_1$| | 1.74176(−3) | 3.156(−18) |
| 0.00 | 1102.662 | 1.104(−4) | 1.054(−4) | 2.019(+5) | 2s2 2p23P0 | 2s2 2p(2P|$_{1/2}^{\rm o}$|) 29d 2[3/2]|$^o_1$| | 1.19101(−3) | 3.963(−17) |
| λobs . | λcalc . | fL . | fV . | Aul . | Lower level . | Upper level . | Iup . | ϵul . |
|---|---|---|---|---|---|---|---|---|
| 0.00 | 1102.557 | 9.358(−5) | 8.937(−5) | 1.712(+5) | 2s2 2p23P0 | 2s2 2p(2P|$_{1/2}^{\rm o}$|) 30d 2[3/2]|$^o_1$| | 1.11253(−3) | 3.355(−17) |
| 0.00 | 1102.558 | 5.455(−6) | 5.345(−6) | 9.977(+3) | 2s2 2p23P0 | 2s2 2p(2P|$_{1/2}^{\rm o}$|) 31s 2[1/2]|$^o_1$| | 1.11343(−3) | 1.955(−18) |
| 0.00 | 1102.617 | 2.550(−5) | 2.430(−5) | 4.663(+4) | 2s2 2p23P0 | 2s2 2p(2P|$_{3/2}^{\rm o}$|) 24d 2[1/2]|$^o_1$| | 1.73510(−3) | 9.266(−18) |
| 0.00 | 1102.618 | 6.034(−5) | 5.792(−5) | 1.103(+5) | 2s2 2p23P0 | 2s2 2p(2P|$_{3/2}^{\rm o}$|) 24d 2[3/2]|$^o_1$| | 1.73617(−3) | 2.192(−17) |
| 0.00 | 1102.626 | 8.681(−6) | 8.180(−6) | 1.588(+4) | 2s2 2p23P0 | 2s2 2p(2P|$_{3/2}^{\rm o}$|) 25s 2[3/2]|$^o_1$| | 1.74176(−3) | 3.156(−18) |
| 0.00 | 1102.662 | 1.104(−4) | 1.054(−4) | 2.019(+5) | 2s2 2p23P0 | 2s2 2p(2P|$_{1/2}^{\rm o}$|) 29d 2[3/2]|$^o_1$| | 1.19101(−3) | 3.963(−17) |
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