HAL Id: jpa-00225417
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Submitted on 1 Jan 1985
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OUR PRESENT UNDERSTANDING OF
DISLOCATION DAMPING
K. Lücke
To cite this version:
JOURNAL DE PHYSIQUE
Colloque C I O , supplément au n012, Tome 46, décembre 1985 page CIO-145
OUR PRESENT UNDERSTANDING OF DISLOCATION DAMPING
K. LUCKE
Institut fiir allgemine Metallkunde and Metallphysik, Ruth,
D-5&QO Aachen,
F. R.
G.For u l t r a - p u r i t y copper t h e d i s l o c a t i o n m o b i l i t y has been i n v e s t i g a t e d by measuring damping and modulus d e f e c t i n t h e MHz- and kHz-range, i n order t o t e s t t h e v a l i d i t y o f t h e d i s l o c a t i o n resonance theory. Electron i r r a d i a t i o n s have been a p p l i e d i n order t o Vary t h e p i n n i n g p o i n t d e n s i t y . I n b o t h frequency ranges i n i t i a l d i f f i c u l t i e s occurred. I n t h e MHz-range a t l o w frequencies, t o o h i g h values were found f o r t h e damping, i n c o n t r a s t t o t h e modulus. It c o u l d be s h o w t h a t these were due t o a s e t o f l o n g l o o p
d i s l o c a t i o n s . I n t h e kHz-range t h e p i n n i n g p o i n t number obtained by damping turned out t o be smaller than t h a t obtained by modulus change. This
discrepancy c o u l d q u a n t i t a t i v e l y be understood by t a k i n g i n t o account d e v i a t i o n s from t h e s t a t i s t i c a l l o o p l e n g t h d i s t r i b u t i o n due t o v i b r a t i o n a l entropy o f t h e d i s l o c a t i o n s and c l u s t e r i n g o f t h e p o i n t d e f e c t s .
The removal o f these two d i f f i c u l t i e s l e d t o a good agreement between t h e data of t h e two frequency ranges wi5h respect t o t h e p i n n i n g behavior. Concerning t h e temperature dependence, A L was found t o have t h e same values i n b o t h ranges which s t r o n g l y increased w i t h temperature. Concerning t h e drag constant B, howev
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r, a s t r o n g disagreement i n both frequency ranges wasobtained ( A and L a r e d e n s i t y and l o o p l e n g t h o f t h e d i s l o c a t i o n s ) . While i n t h e MHz-range t h e drag constant B increased approximately l i n e a r l y w i t h temperature, i t stayed constant i n t h e range between 40 and 350 K i n t h e kHz- range. This shows t h a t two d i f f e r e n t d i s l o c a t i o n drag mechanisms are a c t i n g i n t h i s frequency range. The reasons f o r t h i s behavior a r e not y e t completely c l a r i f i e d .