G. Hancock and I. W. M. Smith, "Quenching of Infrared Chemiluminescence. 1: The Rates of De-Excitation of CO (4 ≤ v ≤ 13) by He, CO, NO, N2, O2, OCS, N2O, and CO2," Appl. Opt. 10, 1827-1842 (1971)
Infrared chemiluminescence has been observed from vibrationally excited CO, formed in the reaction, O + CS → CO + S. The quenching of the CO overtone spectrum has been studied as a function of the concentration of each of a number of added gases. A steady-state treatment is developed which allows rates to be determined for the de-excitation of individual vibrational levels of CO (4 ≤ v ≤ 13) by He, CO (v = 0), NO, N2, O2, OCS, N2O, and CO2. The experimental results are compared with theoretically predicted rates. Finally, the importance of the results for interpreting the behavior of CO vibrational lasers is considered.
You do not have subscription access to this journal. Cited by links are available to subscribers only. You may subscribe either as an Optica member, or as an authorized user of your institution.
You do not have subscription access to this journal. Figure files are available to subscribers only. You may subscribe either as an Optica member, or as an authorized user of your institution.
You do not have subscription access to this journal. Article tables are available to subscribers only. You may subscribe either as an Optica member, or as an authorized user of your institution.
You do not have subscription access to this journal. Equations are available to subscribers only. You may subscribe either as an Optica member, or as an authorized user of your institution.
Pv,v−1 is the probability of de-exciting COv → COv−1 per collision; collision diameters have been taken from Ref. 48.
The upper entry is the rate constant, the lower Pv,v−1; 2.0 (−12) = 2.0 × 10−12.
Calculated from the rate determined for the reverse process.
Estimated from P13,12 and P12,11 for CO–O2, using the slope of the log10(P/v) vs Δν plot for CO–N2 exchange.
Table VI
Reduced Probabilities for CO–N2O and CO–CO2 V-V Exchange
v
νv,v−1
CO–N2O
CO–CO2
4
2064.0
4.0 (−4)
2.5 (−5)
5
2037.7
1.5 (−4)
1.12 (−5)
6
2011.5
7.2 (−5)
9.0 (−6)
7
1985.4
4.1 (−5)
7.3 (−6)
8
1959.3
3.3 (−5)
6.8 (−6)
9
1933.6
2.9 (−5)
7.8 (−6)
10
1907.2
2.9 (−5)
1.12 (−5)
11
1881.7
2.9 (−5)
1.6 (−5)
12
1856.1
2.5 (−5)
2.4 (−5)
13
1829.9
2.1 (−5)
2.1 (−5)
Tables (6)
Table I
Spontaneous Emission Coefficients for CO (sec−1) and Pseudo-First-Order Rate Constants for Self-quenching by Product CO (sec−1)
Av,v−1
Av,v−2
Av,v−3
kv,v−1CO[CO]
v = 1
33.4
—
—
2
64.5
0.9
—
3
92.9
2.8
0.01
4
118.0
5.6
0.05
32
5
142.0
9.3
0.12
21
6
164.3
13.9
0.26
10
7
182.0
19.0
0.45
5.5
8
200.1
25.1
0.7
2.9
9
214.1
32.0
1.1
1.8
10
227.1
39.3
1.6
1.0
11
238.8
47.7
2.3
0.7
12
248.5
56.2
3.1
0.5
13
256.3
65.6
4.1
14
262.5
75.0
5.2
Table II
Rate Constants (cm3 molecule−1 sec−1) and Values of Pv,v−1a for De-excitation of COv by He, CO, NO, O2, N2, OCS, N2O and CO
Pv,v−1 is the probability of de-exciting COv → COv−1 per collision; collision diameters have been taken from Ref. 48.
The upper entry is the rate constant, the lower Pv,v−1; 2.0 (−12) = 2.0 × 10−12.
Calculated from the rate determined for the reverse process.
Estimated from P13,12 and P12,11 for CO–O2, using the slope of the log10(P/v) vs Δν plot for CO–N2 exchange.
Table VI
Reduced Probabilities for CO–N2O and CO–CO2 V-V Exchange