Table 13
Assumed dissociation fraction of NO excited-state vibrational levels.
| Level | Fraction | Reference |
|
|
||
| A(3) a | 0 | Brzozowski et al. (1976) |
| B(6) | 0 | Brzozowski et al. (1976) |
| B(7) b | 0.05 | Brzozowski et al. (1976) |
| B(9) | 0.98 | Hikida & Mori (1978) |
| B(10)c | 1 | |
| B(11)c | 1 | |
| B(12)c | 1 | |
| B(14)c | 1 | |
| C(0) |
|
Brzozowski et al. (1976) |
| C(1)d | 1 | |
| C(2)d | 1 | |
| C(3)d | 1 | |
| D(0) |
|
Luque & Crosley (2000) |
| D(1) |
|
Luque & Crosley (2000) |
| D(2) |
|
Luque & Crosley (2000) |
| D(3) |
|
Luque & Crosley (2000) |
Notes. Level notation as in Yoshino et al. (2006). Rotational angular-momentum quantum number: J.
Dissociates for rotational levels with J> 26, (Brzozowski et al. 1976; Luque & Crosley 2000) but this requires higher temperatures than are relevant here.
This fraction is actually an upper limit (Brzozowski et al. 1974, 1976).
No measurements exist but it is reasonable to expect these levels to dissociate completely because of the large dissociation fraction of the lower-energy level B(9).
Do not appear in emission (Brzozowski et al. 1976).
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