Table 1. Open in new tab Stark widths...

Experimental

Theoretical

Transition^a

Multiplet^a

λ (Å) ^a

w^b

w^c

w^d

w´^d

w^e

3d⁵(⁶S)4s–3d⁵(⁶S)4p

a⁷S–z⁷P^o

2576.104

3.8

9.37

10.1

5.91

2593.721

4.0

16.0

14.0

9.48

10.2

5.91

2605.680

3.7

18.0

14.8

9.67

10.3

5.91

a⁵S–z⁵P^o

2949.205

6.3

15.0

16.0

16.5

13.0

8.51

2939.308

6.3

15.0

12.2

13.6

12.9

8.51

2933.054

6.1

13.0

16.3

13.6

12.9

8.51

3d⁶–3d⁵(⁶S)4p

a⁵D–z⁵P^o

3495.833

11.3

3482.904

11.8

20.0

3488.675

11.0

3d⁵(⁴ G)4s–3d⁵(⁴ G)4p

a⁵G–z⁵G^o

2705.732

5.6

2708.452

4.8

2707.544

4.4

a⁵G–z⁵H^o

2610.200

4.0

8.0

2618.148

4.7

9.2

2625.606

4.7

a⁵G–z⁵F^o

2563.642

4.7

2565.219

3.6

3d⁵(⁴P)4s–3d⁵(⁴ G)4p

a⁵P–z⁵F^o

2716.796

4.7

3d⁵(⁴P)4s–3d⁵(⁴P)4p

a⁵P–z⁵D^o

2672.581

4.5

2724.465

5.0

a⁵P–z⁵S^o

2698.989

5.4

3d⁵(⁴P)4s–3d⁵(⁴D)4p

a⁵P–y⁵D^o

2373.357

3.5

3d⁶–3d⁵(⁴ G)4p

a³H–z³G^o

2507.598

6.8

a³F–z³F^o

2750.126

6.4

3d⁵(⁴D)4s–3d⁵(⁴P)4p

b⁵D–z⁵D^o

2897.068

5.7

b⁵D-y⁵P^o

2816.329

5.8

3d⁵(⁴D)4s–3d⁵(⁴D)4p

b⁵D–y⁵F^o

2639.849

4.4

2677.851

4.5

b⁵D–y⁵D^o

2532.781

4.3

3d⁵(⁴ G)4s–3d⁵(⁴ G)4p

a³G–z³H^o

2886.671

6.3

a³G–z³F^o

2892.389

6.1

a³G–z³G^o

2684.539

5.5

3d⁶–3d⁵(⁴ G)4p

b³G–z³G^o

2815.025

6.9

3d⁵(⁴P)4s–3d⁵(⁴P)4p

b³P–z³P^o

3050.654

6.6

b³P–z³D^o

2900.154

5.9

2891.332

5.8

2885.131

7.0

3d⁶–3d⁵(²I)4p

a¹I–z¹I^o

2320.420

5.7

3d⁵(²I)4s–3d⁵(²I)4p

b¹I–z¹K^o

2870.085

6.9

3d⁵(²F)4s–3d⁵(a ²D)4p

b³F–z¹F^o

2740.786

5.3

3d⁵(² G)4s–3d⁵(a ² G)4p

c³G–x³H^o

2846.036

5.4

Table 1.

Open in new tab

Stark widths (full width at half-maximum, FWHM) w (pm) of Mn ii spectral lines at electron density 10¹⁷ cm⁻³ and for a temperature range of 11 000–13 900 K. The available data in the literature are shown for comparison. The estimated relative error of w is 15 per cent.

				Experimental			Theoretical
No	Transition^a	Multiplet^a	λ (Å) ^a	w	w^b	w^c	w^d	w´^d	w^e
1	3d⁵(⁶S)4s–3d⁵(⁶S)4p	a⁷S–z⁷P^o	2576.104	3.8			9.37	10.1	5.91
			2593.721	4.0	16.0	14.0	9.48	10.2	5.91
			2605.680	3.7	18.0	14.8	9.67	10.3	5.91
2		a⁵S–z⁵P^o	2949.205	6.3	15.0	16.0	16.5	13.0	8.51
			2939.308	6.3	15.0	12.2	13.6	12.9	8.51
			2933.054	6.1	13.0	16.3	13.6	12.9	8.51
3	3d⁶–3d⁵(⁶S)4p	a⁵D–z⁵P^o	3495.833	11.3
			3482.904	11.8	13	20.0
			3488.675	11.0
4	3d⁵(⁴ G)4s–3d⁵(⁴ G)4p	a⁵G–z⁵G^o	2705.732	5.6
			2708.452	4.8
			2707.544	4.4
5		a⁵G–z⁵H^o	2610.200	4.0	13	8.0
			2618.148	4.7		9.2
			2625.606	4.7
6		a⁵G–z⁵F^o	2563.642	4.7
			2565.219	3.6
7	3d⁵(⁴P)4s–3d⁵(⁴ G)4p	a⁵P–z⁵F^o	2716.796	4.7
8	3d⁵(⁴P)4s–3d⁵(⁴P)4p	a⁵P–z⁵D^o	2672.581	4.5
			2724.465	5.0
9		a⁵P–z⁵S^o	2698.989	5.4
10	3d⁵(⁴P)4s–3d⁵(⁴D)4p	a⁵P–y⁵D^o	2373.357	3.5
11	3d⁶–3d⁵(⁴ G)4p	a³H–z³G^o	2507.598	6.8
12		a³F–z³F^o	2750.126	6.4
13	3d⁵(⁴D)4s–3d⁵(⁴P)4p	b⁵D–z⁵D^o	2897.068	5.7
14		b⁵D-y⁵P^o	2816.329	5.8
15	3d⁵(⁴D)4s–3d⁵(⁴D)4p	b⁵D–y⁵F^o	2639.849	4.4
			2677.851	4.5
16		b⁵D–y⁵D^o	2532.781	4.3
17	3d⁵(⁴ G)4s–3d⁵(⁴ G)4p	a³G–z³H^o	2886.671	6.3
18		a³G–z³F^o	2892.389	6.1
19		a³G–z³G^o	2684.539	5.5
20	3d⁶–3d⁵(⁴ G)4p	b³G–z³G^o	2815.025	6.9
21	3d⁵(⁴P)4s–3d⁵(⁴P)4p	b³P–z³P^o	3050.654	6.6
22		b³P–z³D^o	2900.154	5.9
			2891.332	5.8
			2885.131	7.0
23	3d⁶–3d⁵(²I)4p	a¹I–z¹I^o	2320.420	5.7
24	3d⁵(²I)4s–3d⁵(²I)4p	b¹I–z¹K^o	2870.085	6.9
25	3d⁵(²F)4s–3d⁵(a ²D)4p	b³F–z¹F^o	2740.786	5.3
26	3d⁵(² G)4s–3d⁵(a ² G)4p	c³G–x³H^o	2846.036	5.4

				Experimental			Theoretical
No	Transition^a	Multiplet^a	λ (Å) ^a	w	w^b	w^c	w^d	w´^d	w^e
1	3d⁵(⁶S)4s–3d⁵(⁶S)4p	a⁷S–z⁷P^o	2576.104	3.8			9.37	10.1	5.91
			2593.721	4.0	16.0	14.0	9.48	10.2	5.91
			2605.680	3.7	18.0	14.8	9.67	10.3	5.91
2		a⁵S–z⁵P^o	2949.205	6.3	15.0	16.0	16.5	13.0	8.51
			2939.308	6.3	15.0	12.2	13.6	12.9	8.51
			2933.054	6.1	13.0	16.3	13.6	12.9	8.51
3	3d⁶–3d⁵(⁶S)4p	a⁵D–z⁵P^o	3495.833	11.3
			3482.904	11.8	13	20.0
			3488.675	11.0
4	3d⁵(⁴ G)4s–3d⁵(⁴ G)4p	a⁵G–z⁵G^o	2705.732	5.6
			2708.452	4.8
			2707.544	4.4
5		a⁵G–z⁵H^o	2610.200	4.0	13	8.0
			2618.148	4.7		9.2
			2625.606	4.7
6		a⁵G–z⁵F^o	2563.642	4.7
			2565.219	3.6
7	3d⁵(⁴P)4s–3d⁵(⁴ G)4p	a⁵P–z⁵F^o	2716.796	4.7
8	3d⁵(⁴P)4s–3d⁵(⁴P)4p	a⁵P–z⁵D^o	2672.581	4.5
			2724.465	5.0
9		a⁵P–z⁵S^o	2698.989	5.4
10	3d⁵(⁴P)4s–3d⁵(⁴D)4p	a⁵P–y⁵D^o	2373.357	3.5
11	3d⁶–3d⁵(⁴ G)4p	a³H–z³G^o	2507.598	6.8
12		a³F–z³F^o	2750.126	6.4
13	3d⁵(⁴D)4s–3d⁵(⁴P)4p	b⁵D–z⁵D^o	2897.068	5.7
14		b⁵D-y⁵P^o	2816.329	5.8
15	3d⁵(⁴D)4s–3d⁵(⁴D)4p	b⁵D–y⁵F^o	2639.849	4.4
			2677.851	4.5
16		b⁵D–y⁵D^o	2532.781	4.3
17	3d⁵(⁴ G)4s–3d⁵(⁴ G)4p	a³G–z³H^o	2886.671	6.3
18		a³G–z³F^o	2892.389	6.1
19		a³G–z³G^o	2684.539	5.5
20	3d⁶–3d⁵(⁴ G)4p	b³G–z³G^o	2815.025	6.9
21	3d⁵(⁴P)4s–3d⁵(⁴P)4p	b³P–z³P^o	3050.654	6.6
22		b³P–z³D^o	2900.154	5.9
			2891.332	5.8
			2885.131	7.0
23	3d⁶–3d⁵(²I)4p	a¹I–z¹I^o	2320.420	5.7
24	3d⁵(²I)4s–3d⁵(²I)4p	b¹I–z¹K^o	2870.085	6.9
25	3d⁵(²F)4s–3d⁵(a ²D)4p	b³F–z¹F^o	2740.786	5.3
26	3d⁵(² G)4s–3d⁵(a ² G)4p	c³G–x³H^o	2846.036	5.4

^aData from Kramida et al. (2018).

^bBredice et al. (2007). Data reported for a temperature of 10 000 K.

^cDjeniže et al. (2006). Data reported for a temperature of 49 000 K.

^dPopović et al (2008). The w value is calculated including contributions from allowed and forbidden transitions; the w´value is calculated including only dipole allowed transitions. Data reported for a temperature of 10 000 K.

^ePopović & Dimitrijević (1997). Data reported for a temperature of 10 000 K.

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