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HAL Id: jpa-00219234

https://hal.archives-ouvertes.fr/jpa-00219234

Submitted on 1 Jan 1979

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STATIONARY AFTERGLOW STUDY OF THE SINGLY CHARGED ATOMIC IONS IN PURE AR

AND KR

M. Grössl, H. Helm, M. Langenwalter, T.D. Märk

To cite this version:

M. Grössl, H. Helm, M. Langenwalter, T.D. Märk. STATIONARY AFTERGLOW STUDY OF THE

SINGLY CHARGED ATOMIC IONS IN PURE AR AND KR. Journal de Physique Colloques, 1979,

40 (C7), pp.C7-51-C7-52. �10.1051/jphyscol:1979725�. �jpa-00219234�

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JOURNAL D E Ph'YSIQUE CoZZoque C7, suppZdment au n07, Tome 40, JuiZZet 2979, nape C7- 51

STATIONARY AFTEROLOW STUDY OF ME m Y CHARGED ATOMIC IONS I N M E AR AND KR

M. Grossl, H. Helm, M. Langenwalter and T.D. Mark.

I n s t i t u t f. ExperimentaZphysik, Abt. F. exp &rn- n-nd PZasmaphysik, Leopold Franzens U n i v e r s i t t ~ t , A 6020 Innsbruck, Osterreich (Austria).

INTRODUCTION: The t r a n s p o r t phenomena and s t a t e than f o r t h e ground s t a t e i o n . I n r e a c t i o n mechanism of r a r e gas i o n s i n their a d d i t i o n , a strong dependence of the E t a s t a b l e p a r e n t g a s e s have been s t u d i e d with different i o n p o p u l a t i o n on t h e n e u t r a l impurity techniques by a l a r g e number of investigators: c o n c e n t r a t i o n has been observed. Hmever only The q u a n t i t a t i v e knowledge of t r a n s p o r t data one q u a n t i t a t i v e experimental r e s u l t about have been improved enormously by means of t h e r e a c t i v i t y of t h e 2~ i 6 n s t a t e i s

1/2

p r e c i s i o n d r i f t t u b e experiments s o t h a t r e p o r t e d s o f a r . Liu and Conway 19 75 report t h e o r i e s i n c l u d i n g f i n e s t r u c t u r e phencmena a n upper l i m i t , because t h e y cannot t o t a l l y may be t e s t e d . exclude s i d e r e a c t i o n s w i t h i m p u r i t i e s f o r

+ 2 t h e d e s t r u c t i o n frequency of in ( P

N e v e r t h e l e s s , t h e understanding of the reaction in in.

mechanisms i s s t i l l poor. For i n s t a n c e i n EXPERIMENTAL METHOD AND RESULTS: The i o n s argon v a l u e s given i n t h e l i t e r a t u r e for the were produced i n a pulsed hollowcath& glocv e f f e c t i v e 3-body r e a c t i o n r a t e c o e f f i c i e n t discharge and monitored w i t h a mass

f o r t h e conversion of t h e s i n g l y charged meter a s a f u n c t i o n of time a s d e s c r i b e d atomic i o n i n t o t h e dimer i o n elsewhere (Langemalter e t a1.1977). C a r e f u l

( 1 1 ~ r + + 2 A r + A r 2 + + A r a t t e n t i o n was payed t o minimize the inpurity l e v e l i n t h e g a s e s used. Measurements have s c a t t e r between 0.6 and 4 . 7 . 1 0 - ~ ~ a n ~ s - ~ .

been made a t n e u t r a l gas p r e s s u r e s between Hyatt and Kn-tubb 19 72 and Liu and Camay 1975

0 . 3 and 3 T o r r a t 297 K . a t t r i b u t e d an observed a n w l y i n the reaction

behaviour of t h e atomic argon i o n s t o t h e I n A r two d i f f e r e n t e x p o n e n t i a l decays of presence of i o n s i n t h e two f i n e S t ~ U c t u r e t h e Ar'-signal could be observed a t redu&

+ 2

s t a t e s , t h e ground s t a t e A r ( P3,2) and the m e t a s t a b l e s t a t e A ~ * ( ~ P , , ~ ) . A d e f i n i t e d i f f e r e n c e i n r e a c t i v i t y of t h e two f i n e

+ +

s t r u c t u r e s t a t e s of Ne and K r i n t h e i r p a r e n t g a s e s could be observed experimentally i n swarm experiments by Helm and E l f o r d 1978 A s a common evidence a l l m t i o n e d investigators observed a much lower d e s t r u c t i o n efficiency, due t o r e a c t i o n s f o r t h e m e t a s t a b l e i o n i c

gas p r e s s u r e s h i g h e r than 1.6 Torr, as is s h m in Fig. 1 f o r i n s t a n c e . From t h e measurements a t low gas p r e s s u r e s ( < 1 . 5 T o r r ) , where only one e x p o n e n t i a l decay has been observed, a v a l u e f o r t h e zero field nmbility of 1.55 a2/vs could be deduced i n very good agreement with d r i f t tube d a t a . Using t h i s v a l u e e f f e c t i v e 3-body r a t e c o e f f i c i e n t s f o r a l l p r e s s u r e s a r e c a l c u l a t e d and p l o t t e d versus gas pressure

Article published online by EDP Sciences and available at http://dx.doi.org/10.1051/jphyscol:1979725

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( F i g . 2 ) i n a s e m i - l o g a r i t h m i c diagram. The f u l l d o t s , which a r e r e l a t e d e i t h e r t o t h e s i n g l e e x p o n e n t i a l decay mode o r a t h i g h p r e s s u r e s t o t h e f a s t decay d u r i n g t h e e a r l y a f t e r g l o w , l i e between + l o % of a mean v a l u e of t h e r a t e c o e f f i c i e n t of 2 . 4 * 1 0 - ~ ~ c m ~ s - ' . E v i d e n t l y t h i s l o s s r a t e c o r r e s p o n d s t o t h e c o n v e r s i o n p r o c e s s ( 1 ) o f t h e 2 ~ 3 / 2 ground s t a t e i o n s . The open c i r c l e s , c o r r e s p o n d i n g

A r f in Ar

~ ~ ' 2 . 3 1 Torr h2 -

0.162

cm2

tlrne I n

the a f t e r g l o w

F i g . 1 Measured time dependent Ar+ ion current a t high pressures: The double expnential decay curve f o r instance a t po = 2.31 Tarr.

t o t h e slow decay a t h i g h p r e s s u r e s , show a very s t r o n g p r e s s u r e dependence. T h i s slow decay p e r i o d i n t h e l a t e a f t e r g l o w may b e

+ 2

dominated by r e a c t i o n s o f A r ( i o n s f o r which H e l m and Varney 1978 proposed a r e a c t i o n model. F o r t h e i r model the effective 3-body r a t e c o e f f i c i e n t s v e r s u s pressure are

p, in Torr

0 1 2 3

-30 p

I I I

4

J

0

-

0

'a

0 9 0

s A r * in i Ar

D

T - 2 9 7 ~ A'

a 0 162

tmZ

Fi9.Z Effective 3-kfiy r a t e m f f i c i e n t as a function of gas density o r pressure, calm- lated fran the f i r s t ( ) and the second ( o )

decay period of the measured decay curves.

Pressure dependence predicted by H e l m and V m e y f o r the w t a s t a b l e ion state.

we s u s p e c t an a d d i t i o n a l p r o d u c t i o n p r o c e s s by n e u t r a l m e t a s t a b l e - m e t a s t a b l e c o l l i s i o n s .

The s i t u a t i o n i n K r i s s i m i l a r t o A r . The d e r i v e d reduced m o b i l i t y v a l u e is 0.9 cm2/vs.

A 3-body r a t e c o e f f i c i e n t of 2.5- 10-3h6 s-I f o r c o n v e r s i o n of t h e ground s t a t e i o n i n t o t h e m o l e c u l a r i o n h a s b e e n o b t a i n e d .

REFERENCES :

Helm H., Varney R.N. 1978 J.Chem.Phys. 68, 5301

Helm H., Elford M.T. 1978 private ccmnmication Hyatt D., Knewstubb P.F. 1972 Trans.

Faraday soc. 68, 202

Langerwalter M., Wssl M., MSrk T.D. 1977' Proc. XI11 I .C.P.I.G. (Ostberlin) , p. 45 Liu W.F., Comay D.C. 1975~;J.Che~11.Phys. 62, 3070

7 x x N m m :

Research s u p p o r t e d by t h e B s t e r r e i c h i s c h e r Fonds z u r FiSrderung d e r w i s s e n s c h a f t l i c h e n Forschung under P r o j e c t N r . S-18/05.

shown by t h e f u l l l i n e . From t h e p r e s s u r e

b e h a v i o u r o b s e r v e d i n t h e p r e s e n t e x p r i m e n t

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