A detailed discussion of the N2(C 3IIu) and N2(X 1Σg+) vibrational temperatures in N2 glow discharges

被引:31
作者
Levaton, J [1 ]
Amorim, J
Monna, V
Nagai, J
Ricard, A
机构
[1] Univ Fed Santa Catarina, LABMAT, BR-88040900 Florianopolis, SC, Brazil
[2] Ctr Tecn Aeroesp, Inst Tecnol Aeronaut, Dept Fis, BR-12228900 Sao Jose Dos Campos, Brazil
[3] Univ Toulouse 3, CPAT, F-31062 Toulouse, France
关键词
D O I
10.1051/epjap:2004015
中图分类号
O59 [应用物理学];
学科分类号
摘要
A N-2 direct current discharge was studied by optical emission spectroscopy. Experimental parameters as gas How rate (Q), pressure (p) and current (1) were varied independently, covering the following range: 10 < I < 75 mA, 100 < Q < 1000 sccm and 1.7 < p < 10 torr, corresponding to the following plasma parameters: electron density in the range 10(9)-10(12) cm(-3) and reduced electric field between 3 x 10(-16) and 10(-15) V cm(-2). The N-2 (C (IIu)-I-3, upsilon'), N-2(X (1)Sigma(g)(+), upsilon) vibrational temperatures and the gas temperature were obtained from the first and second positive systems emissions. The N-2 (C (IIu)-I-3, upsilon') vibrational distributions did not exhibit a Boltzmann character. A linearization process was employed to such distributions allowing us to calculate the N-2(C (IIu)-I-3, upsilon') temperature. The N-2(X (1)Sigma(g)(+), upsilon) temperature was calculated from 9 the N-2(C (IIu)-I-3, upsilon') one on the basis of the Franck-Condon factors. Results and the method of vibrational temperature calculus are presented.
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页码:59 / 64
页数:6
相关论文
共 12 条
[1]  
CAPITELLI M, 1986, TOPICS CURRENT PHYS, P8
[2]   VIBRATIONAL-RELAXATION OF N2(C,UPSILON)-STATE IN N2 PULSED RF DISCHARGE - ELECTRON-IMPACT AND POOLING REACTIONS [J].
DEBENEDICTIS, S ;
DILECCE, G .
CHEMICAL PHYSICS, 1995, 192 (02) :149-162
[3]  
Herzberg G., 1950, Molecular spectra molecular structure: Spectra of diatomic molecules, V2nd ed.
[4]  
HOCHARD L, 1994, ESCAMPIG E, V108, P336
[5]  
KIOHARA V, 2003, MEASUREMENTS N 2D DE
[6]   Kinetics of atoms, metastable, radiative and ionic species in the nitrogen pink afterglow [J].
Levaton, J ;
Amorim, J ;
Souza, AR ;
Franco, D ;
Ricard, A .
JOURNAL OF PHYSICS D-APPLIED PHYSICS, 2002, 35 (07) :689-699
[7]   COUPLED ELECTRON-ENERGY AND VIBRATIONAL DISTRIBUTION-FUNCTIONS IN STATIONARY N-2 DISCHARGES [J].
LOUREIRO, J ;
FERREIRA, CM .
JOURNAL OF PHYSICS D-APPLIED PHYSICS, 1986, 19 (01) :17-35
[8]   ELECTRON AND VIBRATIONAL KINETICS IN AN N2-H2 GLOW-DISCHARGE WITH APPLICATION TO SURFACE PROCESSES [J].
LOUREIRO, J ;
RICARD, A .
JOURNAL OF PHYSICS D-APPLIED PHYSICS, 1993, 26 (02) :163-176
[9]   Role of long-lived N2(X1Σ+g, υ) molecules and N2(A3Σ+u) and N2(a'1Σ-u) states in the light emissions of an N2 afterglow [J].
Loureiro, J ;
Sá, PA ;
Guerra, V .
JOURNAL OF PHYSICS D-APPLIED PHYSICS, 2001, 34 (12) :1769-1778
[10]   Density of N2 (X 1Σ+g; υ=18) molecules in a dc glow discharge measured by cavity ringdown spectroscopy at 227 nm; validity domain of the technique [J].
Macko, P ;
Cunge, G ;
Sadeghi, N .
JOURNAL OF PHYSICS D-APPLIED PHYSICS, 2001, 34 (12) :1807-1811