TABLE II. Spectral positions of the rotational spectral lines (in nanometers), which belong to the (^-branch of the (()-()). (1-1). and (2-2) bands of the Fulcher-a system of H,.
Transition Q\ Q2 Q7> Q4 Q5 Q6
(0-0) 601.83 602.38 603.19 604.27 605.61 607.20
(1-1) 612.18 612.72 613.54 614.62 615.96
(2-2) 622.48 623.03 623.84 624.92 626.25
Table 1. Rate coefficients (cm1 s" ■ i of the direct and dissociative excitation of the H„ and    lines by electron impact calculated using a Maxwell EEDF at various electron temperatures Tt. The calculated data are given for the a« when redistribution of populations can be neglected (case 1) and in the case of a Boltzmaim distribution over the fine structure sublevels (case 2).
Direct excitation
Dissociative excitation
T< (eV) Cm
Case 2
4.97E-20 1.15E-14 7.03E-13 5.43E-12 1.84E-1I 4.I4E-11 7.38E-U 1.14E-10 1.60E-10 2.09E-10 2.6 IE 10 3.14E-10 3.68E-10 4.21E-10 4.74E-10 S.26E-10 5.77E-10 6.27E-10 6.75E-10 7.22E-10 8.12E-10 8.96E-10 9.76E-10 1.05E-09 1.18E-09 1.30E-09 1.41E-09 1.63E-09 1.79E-09 2.03E-09 2.18E-09 2.39E-09 2.4NU 09
.VI
i: j
i"
5
1.
2. M
4.« 6.1f
7.:
9
2]
4
98|
2.:
2.« 2.:
2. ' 3.1
3. :
3. J 3.81 4.03
4. < 4.'. 4.5J
Case 2		
21	3.93E-	21
13	1.70E-	13
13	1.26E-	13
12	1.07E-	12
12	3.82E-	12
11	8.86E-	12
11	1.61E-	11
11	2.53E-	11
11	3.58E-	11
•ll	4.73E-	11
11	5.94E-	11
11	7.19E-	11
10	8.45E-	11
10	9.71E-	11
10	1.10E-	10
10	1.22E-	10
10	1.34E-	10
10	1.46E-	10
JO	1.57E-	10
lo	1.68E-	10
10	1.89E-	10
10	2.09E-	10
10	2.28E-	10
10	2.45E-	10
10	2.77E-	10
10	3.05E-	10
10	3.29E-	10
10	3.79E-	10
10	4.I8E-	10
10	4.7IE-	10
10	5.05E-	10
10	5.48E-	10
10	5.64E-	10
Case 2		
25	2.63E-	25
17	5.94E-	IS
15	1.77E-	15
14	3.06E-	14
13	1.69E-	13
12	5.28E-	13
12	I.19E-	12
12	2.20E-	12
12	3.55E-	12
11	5.21E-	12
11	7.15E-	12
11	9.32E-	12
11	1.17E-	11
11	1.42E-	11
\ 1	1.69E-	11
11	1.%E-	11
11	2.24E-	11
11	2.53E-	11
11	2.82E-	11
11	3.11E-	11
11	3.71E-	11
11	4.30E-	11
10	4.88E-	11
10	5.46E-	11
10	6.57E-	11
10	7.64E-	11
10	8.64E-	11
10	1.09E-	10
10	1.28E-	10
10	1.58E-	10
10	1.79E-	10
10	2.08E-	10
10	2.22E-	10
Case 2
-26
IK 16
-15 IE—14 -13 13 13 -13 E-12 -12 12 12 12 12 12 12 12 12 1
-1 DE-1 2-1
1
-1 JE-1 i4e-1 -1 1 1 1 1
2.90E-
1.10E
3.65E-
6.55E-
3.68E-
1.17E-
2.68E-
5.03E-
8.26E-
1.24E-
1.73E-
2.31E-
2.95E-
3.65E-
4.42E-
5.23E-
6.08E-
6%E-
7.88E-
8.8 IE-
1.08E-
1.28E-
1.48E-
1.69E-
2.09E-
2.48E-
2.85E-
3.69E-
4.39E-
5.46E-
6.19E-
7.14E-
7.48E-
2^ 19 17 16
13
14 14 14 14
13 13 13 13 13 13 13 13 13 13 13 12 12 12 12 12 12 12 12 12 12 12 12 12
Table 2. Rate coefficients      (cm1 s ') for the excitation of the J JI"I, , v = 2. N = 1 level of molecular hydrogen by electron impact from the ground electronic-vibronic state, calculated using a Maxwellian EEDF at various electron temperatures Tc multipUed with the radiative lifetime of this state r^-2i and the radiative transition probabilities A^j21 of the transition J iT\^, v = 2. N = 1    a3SJ, v = 2, N = 1.
7-e(eV)   A^'r^K^   Tc (eV)   A'j> t^K'^   Tc(eV) Cv2,^
0.5	1.06E-22	6	1.94E-11	14	4.19E-1
1	2.10E-16	6.5	222E-11	16	4.26E-1
1.5	2.45E-14	7	248E-11	IS	4.24E-1
2	2J4E-13	7.5	273E-U	20	4.1 HE 1
2.5	IjOOE-12	8	2.9411 11	25	3.91E-1
3	2.46E-12	8.5	3.14E-11	30	3.58E-1
3.5	458E-12	9	3.32E-M	40	2.99E-1
4	721E-12	9.5	3.47E-11	5(1	2.5 IE-1
4.5	1.02E-11	10	3.61E-U	75	1.72E-1
5	1J3E-11	11	3.83E-11	100	1.27E-1
5.5	1.64E-11	12	4.00E-11		
[H]/[H2] Tf [eV]
Figure 4. The ratio of mtensities of H„ and    lines /H„ / ^ as Figure 5. The ratio of intensities of H, and Hp lines /H„ //H, as
function of the density ratio of atomic and molecular hydrogen, function of Tf1 calculated formations ratios of densities of atomic
calculated for case 2 at various Tf. and molecular hydrogen (i — [HJ/CHJ) for case 2.
Ha {2-2)0,1
	..........		
1000 ■		0.5 eV,	f    /   * " y.-' .'■ *'// '
100 -	WOeV^		V'
	"50eV~/	St t!	\ i
10		/ '5eV	20 eV
1 ■	. "leV		
t0J     Iff1     10''     10° 10'
[tf]/[tf2]
Figure 7, The ratio of intensities of Ho and<2-2)QI lines In. //c-2)oi as a function of the density ratio of atomic and molecular hydrogen [H]/[Hi], calculated forcase 2at various 7^* and Tf = 1000 K_
Ha ' *t,2-2)Q!
1000-		-
		
100-	■,   'v-.._k = 1	
10	k=0.1	^ -
1 ■	^k = 0.01 .jT	-
0.1	/     k = 0.001	-
0.01	/k=0	
1 10 100
Tf [eV]
Figure 8. The ratio of intensities of H„ and(2-2)QI lines Its. /la-DQt 45 a function of Tf calculated for various ratios of densities of atomic and molecular hydrogen (i = [HJ/tBj]) at a Tt - 1000 K.