The (0,O) sequence of the violet (B '2-X' 2) band system of CN produced by the elcctran impact dis.so&tive cxcitatiar. (200 eVI of HCN, BrCN and CzNz was measured. From the rektivc intensities of the R( 14) lines split by rotation4 pertiubatian. the ratio of the formation rate of the A2fl state to
Formation of CN(B2Σ) by the electron impact dissociation of cyanides. Rotational energy distribution of CN(B2Σ) from HCN
✍ Scribed by Ikuo Tokue; Kozo Kuchitsu
- Publisher
- Elsevier Science
- Year
- 1975
- Tongue
- English
- Weight
- 414 KB
- Volume
- 34
- Category
- Article
- ISSN
- 0009-2614
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✦ Synopsis
The rotational structures of the (0,O) sequence of the violet (B "_-X'.Z) band system of CN produced by the electronimpact dissociative excitation of HCN were measured under such conditions that secondary reactions czn be disregrded. The distribution of the spectral intensity was essentially independent of the electron ener_w (80-300 ev). The rotational energy distributions of the Y' = 0,11, I2 and 13 levels of the I3 ' C state can be approximated by two Boltzmann functions; the intensities for higher K fit the distribution for effective temperatures of 1080-1500 K, uld those for lower K for 300-350 K. The formation mechanisms of the CN(B * Z) are discussed.
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Emission spectra of the CN violet band system (B \*Z-X \*S) were observed by the eIectron impact on HCN with seberal impact ener@s near me thieshold. The formation of CN(B) by the dissotiti~ excitation of HCN m invest&t&-The -hoId eneey weed essentiaUy with that obt&ned by the photodissociation meas
The violet emission spectrum (B\* Z-X' C) of the CN radical observed by the collision of HCN with metastable AI(~P, ?) atoms was analyzed. The effective rotational temperature of the CN(B2C) radical, 3s estimated from a band e&elope analysis, is about 2000°K. The disrributions of the excess energy t