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HAL Id: jpa-00219212

https://hal.archives-ouvertes.fr/jpa-00219212

Submitted on 1 Jan 1979

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INFLUENCE OF PERTURBATION ON

POPULATION PROCESSES OF 4p ARGON LEVELS

S. Djeniže, J.M. Labat

To cite this version:

S. Djeniže, J.M. Labat. INFLUENCE OF PERTURBATION ON POPULATION PROCESSES OF 4p ARGON LEVELS. Journal de Physique Colloques, 1979, 40 (C7), pp.C7-47-C7-48.

�10.1051/jphyscol:1979723�. �jpa-00219212�

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JOURNAL DE PHYSIQUE CoZZoque C7, suppZ6rnent au n07, Tome 40, JuiZZet 1979, page C7- 47

INFLUENCE OF PERTURBATION

ON

POPULATION PROCESSES OF 4p ARGON LEVELS

S. DjeniYe and J.M. Labat.

Department of Physics and Meteorology and I n s t i t u t e o f Physics, 11000 Beograd, YugosZavia.

Population of argon 4p levels in a decaying plasma was found to be predominan- tly due to the dissociative recombination of molecular argon ions

(').

This se- lective process of population was sugges- ted by Lorents(3), although no special di- fference between the various 4p levels has been pointed out.

An attempt was made in this study to develop the 4p levels population problem further. For this purpose four spectral lines were selected and their intensities were monitored in a DC regime as well as during the decay of a perturbed argon plasma. Rather interesting behaviour of population densities for the various per- turbation energy was found, although the linear dependence of population on the gas pressure was recorded. Highest 4p level

(upper level of the 7503,37

(a

line) was practicaly under all conditions more' popu- lated in decaying plasma, what was not the case for the lower lying upper level of 8115,31 2 line.

Experiment. The main discharge was driven between the water cooled electrodes

in a special U-shaped tube. Part of the po- sitive column of

4.5

cm length was pertur- bed by an electric pulse applied to two ring electrodes immersed in the plasma.

Short, approximately 3 ns pulses were sup- plied in a repetitive fashion from the Blumlein line of capacitance 2180 pF. The line was charged to 5, 6 and 8 kV, what gives, supposing about 80% of energy is transfered to plasma, the values of per- turbation energies 2.2 3.1.10-~ and 5.6 Joule. Continous flow of the spec- troscopicaly pure argon was sustained at 16 liters per minute. Spectral lines were selected by Zeiss SPM 2 monochromator and recorded using

EM1 9569B

photomultiplier directly coupled to Tektronix 7704 oscillo- scope, or for DC regime to galvanometer.

levels of argon, four spectral lines were selected: two of them originating from tran- sitions between primed levels (7503 ,a7 2

and 7948,18 8; corresponding transitions in the Pashen notation are ls2-2p1 and Is3-2p4) and also two from the other set of levels

(7514,65

(a

and 8115,31 2 from transitions ls4-2p5 and l s 5 - 2 ~ ~ ) . Energy difference between highest 2pl and lowest 2p9 levels is 3260 crn-l or 0.404 eV.

Short perturbation pulse applied to a plasma will cause initialy a rapid line

intensity enhancement. This first peak la- sted for some tens of nanoseconds.* All the lines from 4p to 4s transitions have a se- cond intensity max-imum, 0.5 to 1 us later depending on the pressure(4). Intensity measurements were done at the second maxi- mum. Typical results for population of the four levels in relative units versus pre- ssure with perturbation energy as a para- meter are given in figures 1 and 2.

Results. In order to find the more detailed information on population of 4p

Figure

1

Article published online by EDP Sciences and available at http://dx.doi.org/10.1051/jphyscol:1979723

(3)

p(T0r r )

Figure 2.

Rations of populations of highest 2pl and lowest 2pg levels for DC plasma and for the perturbed plasma versus pressure are given in figure 3, perturbation energy being a parameter.

While the population densities of 2pl level in the whole pressure range are higher than in DC, population of low 2pg level reaches the DC population just at higher pressure and maximum perturbation energy.

Ratios of DC to pulse population pre- sented in figure 3 reveals clearly that the high 2pl level is practicaly always more populated in a decaying plasma. There are probably the favourable conditions for molecular ions formation under these con- ditions. Comparison of population densi- ties of all the 2p levels observed in a decaying plasma shows that 2p5 level be- comes the hoghest populated level in the case of 10 Torr pressure and high pertur- bation energy, although in all the other cases the 2pl level population is predo- minant.

References

1. G.N.Gerasimov, S.Ia.Petrov and I.L.

Sabirova, Optika i Spektroskopia,

42

(1977) 1035 (in russian)

2. Y.J.Shin and M.A.Biondi Phys.Rev. 17 (1978) 868 3. D.C.Lorents

Physica 82C (1976) 19

4. J.M.Labat, J.Vukibevib,

0.

~ a b a t and S. DjeniZe

(this Proceedings).

Figure

3 .

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