Angular correlation and lifetime measurements in 30Si using a Ge(Li) detector

1967 ◽  
Vol 90 (2) ◽  
pp. 321-333 ◽  
Author(s):  
C. Broude ◽  
P.J.M. Smulders ◽  
T.K. Alexander
1968 ◽  
Vol 111 (1) ◽  
pp. 529-550
Author(s):  
W KUTSCHERA ◽  
D PELTE ◽  
G SCHRIEDER

1996 ◽  
Vol 54 (21) ◽  
pp. 15051-15055 ◽  
Author(s):  
S. Dannefaer ◽  
T. Friessnegg ◽  
D. Kerr ◽  
Akira Uedono ◽  
Xiaohe Li ◽  
...  

1968 ◽  
Vol 111 (3) ◽  
pp. 529-550
Author(s):  
W. Kutschera ◽  
D. Pelte ◽  
G. Schrieder

1970 ◽  
Vol 146 (1) ◽  
pp. 99-111 ◽  
Author(s):  
H.J. Maier ◽  
J.G. Pronko ◽  
C. Rolfs

1976 ◽  
Vol 13 (4) ◽  
pp. 1515-1526 ◽  
Author(s):  
L. K. Fifield ◽  
R. W. Zurmühle ◽  
D. P. Balamuth ◽  
S. L. Tabor

1972 ◽  
Vol 50 (14) ◽  
pp. 1619-1622 ◽  
Author(s):  
G. DeBlonde ◽  
S. Y. Chuang ◽  
B. G. Hogg ◽  
D. P. Kerr ◽  
D. M. Miller

In previous experiments with positrons annihilating in liquid organic materials (Hogg et al.) the measurements of IN (intensity of the low momentum component from angular correlation data) and I2 (intensity of the long lived component from lifetime measurements) have resulted in IN = I2/3 within experimental error.For samples of CH4, C6H6, and C6H12 measurements in the liquid state yield the expected equality between IN and I2/3. However, in the solid state for these substances there is a marked disagreement between IN and I2/3. The value of IN, in all cases, is essentially zero suggesting that no positronium is formed, but the value of I2 remains large.


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