Table 5. Open in new tab Comparison of...

Level	λ (Å)	f_L	f_L	f_L
2s²2p (²P\|$_{1/2}^{\rm ^{ o}}$\|⁠) 5d [5/2]	1159.0	2.04(−3)	2.03(−3)	1.90(−3)
2s²2p (²P\|$_{3/2}^{\rm o}$\|⁠) 5d [5/2]	1158.0	1.57(−2)	1.58(−2)	1.59(−2)
2s²2p (²P\|$_{3/2}^{\rm o}$\|⁠) 5d [7/2]	1157.4	1.12(−3)	1.12(−3)	1.12(−3)
2s²2p (²P\|$_{1/2}^{\rm o}$\|⁠) 6d [5/2]	1140.7	1.72(−3)	1.72(−3)	1.67(−3)
2s²2p (²P\|$_{3/2}^{\rm o}$\|⁠) 6d [5/2]	1139.9	8.07(−3)	8.18(−3)	8.21(−3)
2s²2p (²P\|$_{3/2}^{\rm o}$\|⁠) 6d [7/2]	1139.5	1.17(−3)	1.17(−3)	1.18(−3)
2s²2p (²P\|$_{1/2}^{\rm o}$\|⁠) 7d [5/2]	1130.0	1.30(−3)	1.29(−3)	1.29(−3)
2s²2p (²P\|$_{3/2}^{\rm o}$\|⁠) 7d [5/2]	1129.2	4.56(−3)	4.55(−3)	4.63(−3)
2s²2p (²P\|$_{3/2}^{\rm o}$\|⁠) 7d [7/2]	1129.0	1.06(−3)	1.07(−3)	1.07(−3)
2s²2p (²P\|$_{1/2}^{\rm o}$\|⁠) 8d [5/2]	1123.2	9.47(−4)	9.53(−4)	9.53(−4)
2s²2p (²P\|$_{3/2}^{\rm o}$\|⁠) 8d [5/2]	1122.5	2.80(−3)	2.80(−3)	2.84(−3)
2s²2p (²P\|$_{3/2}^{\rm o}$\|⁠) 8d [7/2]	1122.3	8.93(−4)	8.99(−4)	8.96(−4)
2s²2p (²P\|$_{1/2}^{\rm o}$\|⁠) 9d [5/2]	1118.6	6.93(−4)	1.05(−3)	7.01(−4)
2s²2p (²P\|$_{3/2}^{\rm o}$\|⁠) 9d [5/2]	1117.9	1.84(−3)	3.15(−3)	1.86(−3)
2s²2p (²P\|$_{3/2}^{\rm o}$\|⁠) 9d [7/2]	1117.8	7.27(−4)	6.03(−4)	7.30(−4)

Level

λ (Å)

f_L

2s²2p (²P|$_{1/2}^{\rm ^{ o}}$|⁠) 5d [5/2]

1159.0

2.04(−3)

2.03(−3)

1.90(−3)

2s²2p (²P|$_{3/2}^{\rm o}$|⁠) 5d [5/2]

1158.0

1.57(−2)

1.58(−2)

1.59(−2)

2s²2p (²P|$_{3/2}^{\rm o}$|⁠) 5d [7/2]

1157.4

1.12(−3)

2s²2p (²P|$_{1/2}^{\rm o}$|⁠) 6d [5/2]

1140.7

1.72(−3)

1.67(−3)

2s²2p (²P|$_{3/2}^{\rm o}$|⁠) 6d [5/2]

1139.9

8.07(−3)

8.18(−3)

8.21(−3)

2s²2p (²P|$_{3/2}^{\rm o}$|⁠) 6d [7/2]

1139.5

1.17(−3)

1.18(−3)

2s²2p (²P|$_{1/2}^{\rm o}$|⁠) 7d [5/2]

1130.0

1.30(−3)

1.29(−3)

2s²2p (²P|$_{3/2}^{\rm o}$|⁠) 7d [5/2]

1129.2

4.56(−3)

4.55(−3)

4.63(−3)

2s²2p (²P|$_{3/2}^{\rm o}$|⁠) 7d [7/2]

1129.0

1.06(−3)

1.07(−3)

2s²2p (²P|$_{1/2}^{\rm o}$|⁠) 8d [5/2]

1123.2

9.47(−4)

9.53(−4)

2s²2p (²P|$_{3/2}^{\rm o}$|⁠) 8d [5/2]

1122.5

2.80(−3)

2.84(−3)

2s²2p (²P|$_{3/2}^{\rm o}$|⁠) 8d [7/2]

1122.3

8.93(−4)

8.99(−4)

8.96(−4)

2s²2p (²P|$_{1/2}^{\rm o}$|⁠) 9d [5/2]

1118.6

6.93(−4)

1.05(−3)

7.01(−4)

2s²2p (²P|$_{3/2}^{\rm o}$|⁠) 9d [5/2]

1117.9

1.84(−3)

3.15(−3)

1.86(−3)

2s²2p (²P|$_{3/2}^{\rm o}$|⁠) 9d [7/2]

1117.8

7.27(−4)

6.03(−4)

7.30(−4)

Level	λ (Å)	f_L	f_L	f_L
2s²2p (²P\|$_{1/2}^{\rm ^{ o}}$\|⁠) 5d [5/2]	1159.0	2.04(−3)	2.03(−3)	1.90(−3)
2s²2p (²P\|$_{3/2}^{\rm o}$\|⁠) 5d [5/2]	1158.0	1.57(−2)	1.58(−2)	1.59(−2)
2s²2p (²P\|$_{3/2}^{\rm o}$\|⁠) 5d [7/2]	1157.4	1.12(−3)	1.12(−3)	1.12(−3)
2s²2p (²P\|$_{1/2}^{\rm o}$\|⁠) 6d [5/2]	1140.7	1.72(−3)	1.72(−3)	1.67(−3)
2s²2p (²P\|$_{3/2}^{\rm o}$\|⁠) 6d [5/2]	1139.9	8.07(−3)	8.18(−3)	8.21(−3)
2s²2p (²P\|$_{3/2}^{\rm o}$\|⁠) 6d [7/2]	1139.5	1.17(−3)	1.17(−3)	1.18(−3)
2s²2p (²P\|$_{1/2}^{\rm o}$\|⁠) 7d [5/2]	1130.0	1.30(−3)	1.29(−3)	1.29(−3)
2s²2p (²P\|$_{3/2}^{\rm o}$\|⁠) 7d [5/2]	1129.2	4.56(−3)	4.55(−3)	4.63(−3)
2s²2p (²P\|$_{3/2}^{\rm o}$\|⁠) 7d [7/2]	1129.0	1.06(−3)	1.07(−3)	1.07(−3)
2s²2p (²P\|$_{1/2}^{\rm o}$\|⁠) 8d [5/2]	1123.2	9.47(−4)	9.53(−4)	9.53(−4)
2s²2p (²P\|$_{3/2}^{\rm o}$\|⁠) 8d [5/2]	1122.5	2.80(−3)	2.80(−3)	2.84(−3)
2s²2p (²P\|$_{3/2}^{\rm o}$\|⁠) 8d [7/2]	1122.3	8.93(−4)	8.99(−4)	8.96(−4)
2s²2p (²P\|$_{1/2}^{\rm o}$\|⁠) 9d [5/2]	1118.6	6.93(−4)	1.05(−3)	7.01(−4)
2s²2p (²P\|$_{3/2}^{\rm o}$\|⁠) 9d [5/2]	1117.9	1.84(−3)	3.15(−3)	1.86(−3)
2s²2p (²P\|$_{3/2}^{\rm o}$\|⁠) 9d [7/2]	1117.8	7.27(−4)	6.03(−4)	7.30(−4)

Table 5.

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Comparison of absorption oscillator strengths in the length formulation for 2s² 2p² ³P₂–2s² 2p nd (J = 3^o) transitions with 5 ≤ n ≤ 9 from Zatsarinny & Froese Fischer (2002), (ZF), the compilation of Haris & Kramida (2017), (HK) and the present work (PW). For n ≤ 8, Haris & Kramida (2017) quote the calculations of Tachiev & Froese Fischer (2001). For n = 9 and higher they report their own calculations using the code described by Cowan (1981).

Level	λ (Å)	f_L	f_L	f_L
		ZF	HK	PW
2s²2p (²P\|$_{1/2}^{\rm ^{ o}}$\|⁠) 5d [5/2]	1159.0	2.04(−3)	2.03(−3)	1.90(−3)
2s²2p (²P\|$_{3/2}^{\rm o}$\|⁠) 5d [5/2]	1158.0	1.57(−2)	1.58(−2)	1.59(−2)
2s²2p (²P\|$_{3/2}^{\rm o}$\|⁠) 5d [7/2]	1157.4	1.12(−3)	1.12(−3)	1.12(−3)
2s²2p (²P\|$_{1/2}^{\rm o}$\|⁠) 6d [5/2]	1140.7	1.72(−3)	1.72(−3)	1.67(−3)
2s²2p (²P\|$_{3/2}^{\rm o}$\|⁠) 6d [5/2]	1139.9	8.07(−3)	8.18(−3)	8.21(−3)
2s²2p (²P\|$_{3/2}^{\rm o}$\|⁠) 6d [7/2]	1139.5	1.17(−3)	1.17(−3)	1.18(−3)
2s²2p (²P\|$_{1/2}^{\rm o}$\|⁠) 7d [5/2]	1130.0	1.30(−3)	1.29(−3)	1.29(−3)
2s²2p (²P\|$_{3/2}^{\rm o}$\|⁠) 7d [5/2]	1129.2	4.56(−3)	4.55(−3)	4.63(−3)
2s²2p (²P\|$_{3/2}^{\rm o}$\|⁠) 7d [7/2]	1129.0	1.06(−3)	1.07(−3)	1.07(−3)
2s²2p (²P\|$_{1/2}^{\rm o}$\|⁠) 8d [5/2]	1123.2	9.47(−4)	9.53(−4)	9.53(−4)
2s²2p (²P\|$_{3/2}^{\rm o}$\|⁠) 8d [5/2]	1122.5	2.80(−3)	2.80(−3)	2.84(−3)
2s²2p (²P\|$_{3/2}^{\rm o}$\|⁠) 8d [7/2]	1122.3	8.93(−4)	8.99(−4)	8.96(−4)
2s²2p (²P\|$_{1/2}^{\rm o}$\|⁠) 9d [5/2]	1118.6	6.93(−4)	1.05(−3)	7.01(−4)
2s²2p (²P\|$_{3/2}^{\rm o}$\|⁠) 9d [5/2]	1117.9	1.84(−3)	3.15(−3)	1.86(−3)
2s²2p (²P\|$_{3/2}^{\rm o}$\|⁠) 9d [7/2]	1117.8	7.27(−4)	6.03(−4)	7.30(−4)

Level	λ (Å)	f_L	f_L	f_L
		ZF	HK	PW
2s²2p (²P\|$_{1/2}^{\rm ^{ o}}$\|⁠) 5d [5/2]	1159.0	2.04(−3)	2.03(−3)	1.90(−3)
2s²2p (²P\|$_{3/2}^{\rm o}$\|⁠) 5d [5/2]	1158.0	1.57(−2)	1.58(−2)	1.59(−2)
2s²2p (²P\|$_{3/2}^{\rm o}$\|⁠) 5d [7/2]	1157.4	1.12(−3)	1.12(−3)	1.12(−3)
2s²2p (²P\|$_{1/2}^{\rm o}$\|⁠) 6d [5/2]	1140.7	1.72(−3)	1.72(−3)	1.67(−3)
2s²2p (²P\|$_{3/2}^{\rm o}$\|⁠) 6d [5/2]	1139.9	8.07(−3)	8.18(−3)	8.21(−3)
2s²2p (²P\|$_{3/2}^{\rm o}$\|⁠) 6d [7/2]	1139.5	1.17(−3)	1.17(−3)	1.18(−3)
2s²2p (²P\|$_{1/2}^{\rm o}$\|⁠) 7d [5/2]	1130.0	1.30(−3)	1.29(−3)	1.29(−3)
2s²2p (²P\|$_{3/2}^{\rm o}$\|⁠) 7d [5/2]	1129.2	4.56(−3)	4.55(−3)	4.63(−3)
2s²2p (²P\|$_{3/2}^{\rm o}$\|⁠) 7d [7/2]	1129.0	1.06(−3)	1.07(−3)	1.07(−3)
2s²2p (²P\|$_{1/2}^{\rm o}$\|⁠) 8d [5/2]	1123.2	9.47(−4)	9.53(−4)	9.53(−4)
2s²2p (²P\|$_{3/2}^{\rm o}$\|⁠) 8d [5/2]	1122.5	2.80(−3)	2.80(−3)	2.84(−3)
2s²2p (²P\|$_{3/2}^{\rm o}$\|⁠) 8d [7/2]	1122.3	8.93(−4)	8.99(−4)	8.96(−4)
2s²2p (²P\|$_{1/2}^{\rm o}$\|⁠) 9d [5/2]	1118.6	6.93(−4)	1.05(−3)	7.01(−4)
2s²2p (²P\|$_{3/2}^{\rm o}$\|⁠) 9d [5/2]	1117.9	1.84(−3)	3.15(−3)	1.86(−3)
2s²2p (²P\|$_{3/2}^{\rm o}$\|⁠) 9d [7/2]	1117.8	7.27(−4)	6.03(−4)	7.30(−4)

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