Transition wavelengths (λij in Å), radiative rates (Aji in s−1), oscillator strengths (fij, dimensionless) and line strengths (S, in atomic units) for electric dipole (E1), and Aji for E2, M1 and M2 transitions in Si ii (a ± b ≡ a ×10±b). (For complete table see Supporting Information.)
| i . | j . | λij . | |$A^{{\rm E1}}_{ji}$| . | |$f^{{\rm E1}}_{ij}$| . | SE1 . | |$A^{{\rm E2}}_{ji}$| . | |$A^{{\rm M1}}_{ji}$| . | |$A^{{\rm M2}}_{ji}$| . |
|---|---|---|---|---|---|---|---|---|
| 1 | 2 | 3.919+05 | 0.000+00 | 0.000+00 | 0.000+00 | 1.082−09 | 1.494−04 | 0.000+00 |
| 1 | 3 | 2.580+03 | 1.703+03 | 1.700−06 | 2.889−05 | 0.000+00 | 0.000+00 | 0.000+00 |
| 1 | 4 | 2.573+03 | 8.227+00 | 1.634−08 | 2.768−07 | 0.000+00 | 0.000+00 | 2.818−03 |
| 1 | 5 | 2.562+03 | 0.000+00 | 0.000+00 | 0.000+00 | 0.000+00 | 0.000+00 | 1.103−03 |
| 1 | 6 | 1.734+03 | 1.167+05 | 1.051−04 | 1.200−03 | 0.000+00 | 0.000+00 | 3.553−07 |
| 1 | 7 | 1.733+03 | 0.000+00 | 0.000+00 | 0.000+00 | 0.000+00 | 0.000+00 | 2.256−02 |
| 1 | 8 | 1.417+03 | 4.996+08 | 1.503−01 | 1.402+00 | 0.000+00 | 0.000+00 | 0.000+00 |
| 1 | 9 | 1.188+03 | 4.781+08 | 1.012−01 | 7.923−01 | 0.000+00 | 0.000+00 | 0.000+00 |
| 1 | 10 | 1.171+03 | 0.000+00 | 0.000+00 | 0.000+00 | 0.000+00 | 8.890−06 | 0.000+00 |
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| i . | j . | λij . | |$A^{{\rm E1}}_{ji}$| . | |$f^{{\rm E1}}_{ij}$| . | SE1 . | |$A^{{\rm E2}}_{ji}$| . | |$A^{{\rm M1}}_{ji}$| . | |$A^{{\rm M2}}_{ji}$| . |
|---|---|---|---|---|---|---|---|---|
| 1 | 2 | 3.919+05 | 0.000+00 | 0.000+00 | 0.000+00 | 1.082−09 | 1.494−04 | 0.000+00 |
| 1 | 3 | 2.580+03 | 1.703+03 | 1.700−06 | 2.889−05 | 0.000+00 | 0.000+00 | 0.000+00 |
| 1 | 4 | 2.573+03 | 8.227+00 | 1.634−08 | 2.768−07 | 0.000+00 | 0.000+00 | 2.818−03 |
| 1 | 5 | 2.562+03 | 0.000+00 | 0.000+00 | 0.000+00 | 0.000+00 | 0.000+00 | 1.103−03 |
| 1 | 6 | 1.734+03 | 1.167+05 | 1.051−04 | 1.200−03 | 0.000+00 | 0.000+00 | 3.553−07 |
| 1 | 7 | 1.733+03 | 0.000+00 | 0.000+00 | 0.000+00 | 0.000+00 | 0.000+00 | 2.256−02 |
| 1 | 8 | 1.417+03 | 4.996+08 | 1.503−01 | 1.402+00 | 0.000+00 | 0.000+00 | 0.000+00 |
| 1 | 9 | 1.188+03 | 4.781+08 | 1.012−01 | 7.923−01 | 0.000+00 | 0.000+00 | 0.000+00 |
| 1 | 10 | 1.171+03 | 0.000+00 | 0.000+00 | 0.000+00 | 0.000+00 | 8.890−06 | 0.000+00 |
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Transition wavelengths (λij in Å), radiative rates (Aji in s−1), oscillator strengths (fij, dimensionless) and line strengths (S, in atomic units) for electric dipole (E1), and Aji for E2, M1 and M2 transitions in Si ii (a ± b ≡ a ×10±b). (For complete table see Supporting Information.)
| i . | j . | λij . | |$A^{{\rm E1}}_{ji}$| . | |$f^{{\rm E1}}_{ij}$| . | SE1 . | |$A^{{\rm E2}}_{ji}$| . | |$A^{{\rm M1}}_{ji}$| . | |$A^{{\rm M2}}_{ji}$| . |
|---|---|---|---|---|---|---|---|---|
| 1 | 2 | 3.919+05 | 0.000+00 | 0.000+00 | 0.000+00 | 1.082−09 | 1.494−04 | 0.000+00 |
| 1 | 3 | 2.580+03 | 1.703+03 | 1.700−06 | 2.889−05 | 0.000+00 | 0.000+00 | 0.000+00 |
| 1 | 4 | 2.573+03 | 8.227+00 | 1.634−08 | 2.768−07 | 0.000+00 | 0.000+00 | 2.818−03 |
| 1 | 5 | 2.562+03 | 0.000+00 | 0.000+00 | 0.000+00 | 0.000+00 | 0.000+00 | 1.103−03 |
| 1 | 6 | 1.734+03 | 1.167+05 | 1.051−04 | 1.200−03 | 0.000+00 | 0.000+00 | 3.553−07 |
| 1 | 7 | 1.733+03 | 0.000+00 | 0.000+00 | 0.000+00 | 0.000+00 | 0.000+00 | 2.256−02 |
| 1 | 8 | 1.417+03 | 4.996+08 | 1.503−01 | 1.402+00 | 0.000+00 | 0.000+00 | 0.000+00 |
| 1 | 9 | 1.188+03 | 4.781+08 | 1.012−01 | 7.923−01 | 0.000+00 | 0.000+00 | 0.000+00 |
| 1 | 10 | 1.171+03 | 0.000+00 | 0.000+00 | 0.000+00 | 0.000+00 | 8.890−06 | 0.000+00 |
| . | . | . | . | . | . | . | . | . |
| . | . | . | . | . | . | . | . | . |
| . | . | . | . | . | . | . | . | . |
| i . | j . | λij . | |$A^{{\rm E1}}_{ji}$| . | |$f^{{\rm E1}}_{ij}$| . | SE1 . | |$A^{{\rm E2}}_{ji}$| . | |$A^{{\rm M1}}_{ji}$| . | |$A^{{\rm M2}}_{ji}$| . |
|---|---|---|---|---|---|---|---|---|
| 1 | 2 | 3.919+05 | 0.000+00 | 0.000+00 | 0.000+00 | 1.082−09 | 1.494−04 | 0.000+00 |
| 1 | 3 | 2.580+03 | 1.703+03 | 1.700−06 | 2.889−05 | 0.000+00 | 0.000+00 | 0.000+00 |
| 1 | 4 | 2.573+03 | 8.227+00 | 1.634−08 | 2.768−07 | 0.000+00 | 0.000+00 | 2.818−03 |
| 1 | 5 | 2.562+03 | 0.000+00 | 0.000+00 | 0.000+00 | 0.000+00 | 0.000+00 | 1.103−03 |
| 1 | 6 | 1.734+03 | 1.167+05 | 1.051−04 | 1.200−03 | 0.000+00 | 0.000+00 | 3.553−07 |
| 1 | 7 | 1.733+03 | 0.000+00 | 0.000+00 | 0.000+00 | 0.000+00 | 0.000+00 | 2.256−02 |
| 1 | 8 | 1.417+03 | 4.996+08 | 1.503−01 | 1.402+00 | 0.000+00 | 0.000+00 | 0.000+00 |
| 1 | 9 | 1.188+03 | 4.781+08 | 1.012−01 | 7.923−01 | 0.000+00 | 0.000+00 | 0.000+00 |
| 1 | 10 | 1.171+03 | 0.000+00 | 0.000+00 | 0.000+00 | 0.000+00 | 8.890−06 | 0.000+00 |
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