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HAL Id: jpa-00221562

https://hal.archives-ouvertes.fr/jpa-00221562

Submitted on 1 Jan 1981

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BRILLOUIN SCATTERING IN SILVER HALIDES

T. Hattori, T. Imanishi, H. Kurokawa, A. Mitsuishi

To cite this version:

T. Hattori, T. Imanishi, H. Kurokawa, A. Mitsuishi. BRILLOUIN SCATTERING IN SILVER HALIDES. Journal de Physique Colloques, 1981, 42 (C6), pp.C6-920-C6-922.

�10.1051/jphyscol:19816274�. �jpa-00221562�

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JOURNAL DE PHYSIQUE

Colloque C6, suppZ6ment au n o 22, Tome 4 2 , dkcembre 1981

BRILLOUIN SCATTERING IN SILVER HALIDES

T. H a t t o r i , T . Irnanishi, H. Kurokawa and A. Mitsuishi

Department o f Applied Physics, Osaka University, S u i t a , Osaka 565, Japan

A b s t r a c t .- P o l a r i z e d B r i l l o u i n s c a t t e r i n g s p e c t r a i n AgBr and AgCl c r y s t a l s w e r e m e a s u r e d i n t h e t e m p e r a t u r e r e g i o n f r o m room t e m p e r a t u r e t o l i q u i d p h a s e t e m p e r a t u r e a b o v e t h e m e l t i n g p o i n t . The anomaly t h a t t h e a c o u s t i c phonon f r e q u e n c y shows a marked d e c r e a s e a t h i g h t e m p e r a t u r e c a n n o t b e i n t e r p r e t e d by a q u a s i - h a r m o n i c a p p r o x i m a t i o n . The d i s c u s s i o n i s g i v e n on t h e r e l a t i o n b e t w e e n t h e anomalous f e a t u r e s and t h e i n c r e a s i n g F r e n k e l d e - f e c t s .

1. I n t r o d u c t i o n . - I t i s w e l l known t h a t s i l v e r h a l i d e s show an anomaly i n i o n i c c o n d u c t i v i t y [ 1 ] , l a t t i c e c o n s t a n t [ 2 ] , s p e c i f i c h e a t [ 3 ] and o t h e r s a t h i g h t e m p e r a t u r e . The a n o m a l y i n t h e e l a s t i c c o n s t a n t C l l o f AgBr was o b s e r v e d by u s i n g an u l t r a s o n i c p u l s e t e c h n i q u e [ 4 ] . I t i s g e n e r a l l y assumed t h a t t h i s anomaly i s a s s o c i a t e d w i t h F r e n k e l d e f e c t , b u t t h e r e seems t o b e n o d e t a i l e d d i s c u s s i o n . I n o r d e r t o s t u d y t h e anomaly i n t h e c a s e o f AgBr a n d AgC1, p o l a r i z e d B r i l l o u i n s c a t t e r i n g s p e c t r a were m e a s u r e d i n t h e t e m p e r a t u r e r e g i o n from room t e m p e r a t u r e t o l i q u i d p h a s e t e m p e r a t u r e a b o v e t h e m e l t i n g p o i n t .

2 . E x p e r i m e n t . - S p h e r i c a l s i n g l e c r y s t a l s o f AgRr and AgCl were grown by t h e Bridgman method. The o r i e n t a t i o n o f c r y s t a l was d e t e r m i n e d b y t h e o b s e r v a t i o n o f t h e e t c h p i t s and was c h e c k e d by a Laue X - r a y t e c h - n i q u e . The c r y s t a l s were c u t and p o l i s h e d s o t h a t t h e w a v e v e c t o r c a n b e t r a n s f e r e d a l o n g < l o o > o r < 1 1 0 > d i r e c t i o n s . A f t e r p o l i s h i n g t h e c r y s t a l s were a n n e a l e d a t a b o u t 350°C and t h e n s l o w l y c o o l e d t o room t e m p e r a t u r e . The c r y s t a l f o r t h e o p t i c a l m e a s u r e m e n t s was l o c a t e d i n an e l e c t r i c f u r n a c e w i t h f u s e d q u a r t z - w i n d o w s . F o r t h e m e a s u r e m e n t s a t l i q u i d p h a s e t e m p e r a t u r e , t h e powder o f AgBr o r AgCl s e a l e d i n a s m a l l f u s e d q u a r t z - t u b e i n h i g h vaccum was m e l t e d i n t h e f u r n a c e . 3 . R e s u l t s . - T h r e e modes, w h i c h p a r t i c i p a t e i n t h e e l a s t i c c o n s t a n t s C l l , C 4 4 and 7(Cll+C12+2C44), 1 r e s p e c t i v e l y , w e r e o b s e r v e d i n t h e p o l a - r i s e d B r i l l o u i n s c a t t e r i n g s p e c t r a , w h i c h w e r e m e a s u r e d u s i n g a t r i p l e p a s s p r e s s u r e s c a n n i n g F a b r y - P e r o t i n t e r f e r o m e t e r . The f o l l o w i n g t h r e e v a l u e s f o r t h o s e t h r e e modes w e r e o b t a i n e d a s a f u n c t i o n on tem- p e r a t u r e : t h e v a l u e o f t h e B r i l l o u i n s h i f t , t h e h a l f w i d t h o f t h e

Article published online by EDP Sciences and available at http://dx.doi.org/10.1051/jphyscol:19816274

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B r i l l o u i n band a n d t h e i n t e n s i t y r a t i o ( I L / I T ) o f t h e l o n g i t u d i n a l a c o u s t i c (LA)

phonon t o t h e t r a n s v e r s e a c o u s t i c (TA) phonon. F i g u r e 1 shows t h e t e m p e r a t u r e d e p e n d e n c e o f t h e t h r e e v a l u e s f o r b o t h Cll and C44 modes o f AgBr. Both v a l u e s o f t h e B r i l l o u i n s h i f t f o r C l l a n d C 4 4 modes d e c r e a s e l i n e a r l y w i t h i n c r e a s i n g t e m p e r a t u r e up t o a b o u t 300°C a n d t h e r e - a f t e r show a marked d e c r e a s e t o m e l t i n g p o i n t . T o g e t h e r w i t h t h e phenomea m e n t i o n e d a b o v e , t h e v a l u e o f I L / I T i n -

TA- m o d e ( C ~ & )

. --.

*"

c r e a s e s s l i g h t l y w i t h i n c r e a s i n g t e m p e r a -

t u r e up t o a b o u t 300°C a n d t h e n i n c r e a s e s Excitation 632.8 n

r a p i d l y a s i f i t d i v e r g e s a t t h e m e l t i n g p o i n t . On t h e o t h e r h a n d , t h e s h a p e o f e a c h B r i l l o u i n band i s a L o r e n t z i a n i n

t h e same phenomena a s AgBr was o b s e r v e d . ~ ~ ~ n ~ ; ~ o ~ r ~ ~ ~ ~ ~ ~ f n ~ X ~ ~ O ~ g f

whole t e m p e r a t u r e r e g i o n m e a s u r e d i n c l u d -

4 . D i s c u s s i o n . - I n g e n e r a l , t h e f r e q u e n c y AgBr.

o f a phonon ( w ; ) i s a f u n c t i o n o f t e m p e r a -

. . . ...*.

mp.

t u r e ( T ) a n d volume ( V ) J

.

T h e r e f o r e , i t s d e r i v a t i v e dw. i s e x p r e s s e d

a s f o l l o w s : 3

i n g t h e l i q u i d p h a s e , a n d t h e h a l f w i d t h O loo "O 300 LOO Temperature ('C)

o f 4 x 1 0 - ~ c m - ~ h a r d l y c h a n g e s w i t h i n e x - F i g . l : Temperature d e - p e r i m e n t a l e r r o r s . I n t h e c a s e o f AgC1, p e n d e n c e o f LA a n d TA

Under t h e c o n d i t i o n o f t h e c o n s t a n t p r e s s u r e , E g ( 1 ) c a n be t r a n s f e r e d

w h e r e , a i s t h e c o e f f i c i e n t o f volume t h e r m a l e x p a n s i o n and y . t h e

mode- runei is en p a r a m e t e r , r e s p e c t i v e l y . I n s i l v e r h a l i d e s , b o t h J p h y s i c a l c o n s t n a n t s o f a and y . w e r e o b t a i n e d by Lawson e t a 1 . [ 2 ] and by L o j e e t a 1 . [ 5 ] , r e s p e c t i v e l y . J T h e r e f o r s , we c a n c a l c u l a t e t h e v a l u e o f t h e f i r s t t e r m o f e q u a t i o n ( 2 ) a s shown i n f i g u r e 2 b y t h e symbol 0 . The s e c o n d t e r m o f e q u a t i o n ( 2 ) shows t h e c o n t r i b u t i o n o f t h e a n h a r m o n i c i t y . I t i s assumed t h a t t h e c a l c u l a t e d v a l u e o f t h e s e c o n d t e r m i s i n d e p e n d e n t o f t e m p e r a t u r e a n d i s a c o n s t a n t , b e c a u s e

(4)

C6-922 JOURNAL DE PHYSIQUE

o f - - -

, t h e h a l f w i d t h o f e a c h a c o u s t i c phonon

: The c o m p a r i s o n b e t w e e n e q u a t i o n ( 2 ) i n o r d e r t o i n t e r p r e t e

%%xperimental c u r v e ( s o l i d t h i s anomaly.

l i n e ) a n d t h e c a l c u l a t e d o n e s The v a l u e s o f (dN/dT) o f t h e t e m o e r a t u r e d e r i v a t i v e w e r e a l r e a d y r e p o r t e d r 6 1 . B e c a u s e ,

- 2 band h a r d l y c h a n g e s a s shown i n f i g u r e

- 4

- 6 - c,, mode

:\: 1

1. T h e r e f o r e , t h e c a l c u l a t e d c u r v e o f

. .

of t h e phoion frequency f o r t h e v a l u e s

bf

( a w . / a ~ ) c a n n o t m e a s u r e ,

e a c h mode. The d i s c o n t i n u - 1

- 8 - - 1 0 -

-12-

-14

a t i o n o f e a c h c u r v e a t 290°C i t was t a k e n a s a - f i t t i n g p a r a m e t e r . t h e e q u a t i o n ( 2 ) i s a s shown i n f i g u r e 2 b y u s i n g t h e symbol A . T h i s c u r v e d o e s n o t a g r e e w i t h t h e e x p e r i m e n t a l -

, , , c u r v e a t a l l . Namely, t h e anomaly

- .

i s n o t e s s e n t i a l , b e c a u s e i t T h e b e s t f i t value i s 1.5cm-1. And i s d u e t o t h e f a c t t h a t we v u t

dw/dT t o b e c o n s t a n t a t t h e - t h e n , t h e c a l c u l a t e d c u r v e i s o b t a i n e d temperature regi0n u n d e r 2 9 0 0 C a s in f i g u r e 2 b y t h e symbol x . f o r c o n v e n i e n c e o f t h e c a l c u -

-2 t h a t t h e a c o u s t i c phonons show a marked

l a t i o n . S e e t h e t e x t c o n c e r n - T h e r e f o r e , i t i s c o n s i d e r e d t h a t t h e

-

-1

- 'k - 6 - v

r5

-,-

7% -10-

5 -12-

ql- -11- V ‘ O

t - 0'- - 2 - L

i n g t h e c a l c u l a t e d c u r v e s .

a n o m a l o u s f e a t u r e s o f t h e a c o u s t i c phonon o f s i l v e r h a l i d e s c a n b e i n t e r p r e t e d v e r y w e l l by t h e t h i r d

0 " 200 1 Ternperature("C -"I300 ) &OD

1

t r a t i o n o f F r e n k e l d e f e c t , J i s a d d e d i n

- ;:oo

\ 1

d e c r e a s e a t h i g h t e m p e r a t u r e c a n n o t b e

t e r m a d d e d n e w l y i n e q u a t i o n ( 2 ) . The same a n a l y s i s i s made f o r t h e

~'rnodc c~=$(c,.c,,.~c,,)

.

-

-

I

c a s e o f AgC1. To c l a r i f y t h e t h i r d term, f u r t h e r s t u d y i s i n p r o g r e s s . i n t e r p r e t e d by a q u a s i h a r m o n i c a p p r o x i - m a t i o n . And t h i s a n o m a l y was o b s e r v e d f o r a l l a c o u s t i c phonon modes. I t i s c o n s i d e r e d t h a t t h e i n c r e a s i n g F r e n k e l

*Work s u p p o r t e d i n p a r t by G r a n t - i n - A i d f o r S c i e n t i f i c R e s e a r c h , t h e M i n i s t r y o f E d u c a t i o n , J a p a n .

Ccrmode d e f e c t a t h i g h t e m p e r a t u r e p l a y e s a

O O . , O O O O O . ~ O O

...

I . 4 d o m i n a n t r o l e i n t h i s anomalous b e -

- h a v i o r . T h e r e f o r e , t h e t h i r d t e r m a s

- ( a u . / a N ) (dN/dT) , where N i s t h e c o n c e n -

R e f e r e n c e s

[ l ] J.K.Aboagye a n d R . J , F r i a u f , Phys . R e v . , B s ( 1 9 7 5 ) 1 6 5 4 .

[ Z ] A.W.Lawson, P h y s . R e v . , 2 ( 1 9 5 0 ) 1 8 5 .

[ 3 ] W.Jost a n d P . K u b a s c h e w s k i , Z.Phys.Chem.Neue F o l g e 60 (1968)69.

[ 4 ] D. S . T a n n h a u s e r , L . J . B r u n e r a n d A. W.Lawson, Phys .Rev. , 102 ( 1 9 5 6 ) 1276.

[ 5 ] K. F . L o j e a n d D . E . S c h v e l e , J . P h y s . C h e m . S o l i d , 2 ( 1 9 7 0 ) 2 0 5 1 . [ 6 ] F . S e i t z , P h y s . R e v . , 56 ( 1 9 3 9 ) 1 0 6 3 .

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