Shape isomerism and shape coexistence effects on the Coulomb energy differences in theN=Znucleus66As and neighboringT=1multiplets

2012 ◽  
Vol 85 (3) ◽  
Author(s):  
G. de Angelis ◽  
K. T. Wiedemann ◽  
T. Martinez ◽  
R. Orlandi ◽  
A. Petrovici ◽  
...  
1982 ◽  
Vol 114 (6) ◽  
pp. 387-391 ◽  
Author(s):  
I. Ragnarsson ◽  
S. Åberg

1992 ◽  
Vol 68 (26) ◽  
pp. 3853-3856 ◽  
Author(s):  
Y. Xu ◽  
K. S. Krane ◽  
M. A. Gummin ◽  
M. Jarrio ◽  
J. L. Wood ◽  
...  
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2003 ◽  
Vol 67 (9) ◽  
Author(s):  
Jeff Greensite ◽  
Štefan Olejník
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2009 ◽  
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W. D. Kulp ◽  
J. L. Wood ◽  
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S. Choudry ◽  
...  
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2005 ◽  
Vol 72 (2) ◽  
Author(s):  
S. M. Fischer ◽  
T. Anderson ◽  
P. Kerns ◽  
G. Mesoloras ◽  
D. Svelnys ◽  
...  

1964 ◽  
Vol 19 (9) ◽  
pp. 1070-1075
Author(s):  
H. Vogel ◽  
H. Bässler

The activation energy of the d. c. conductance of organic liquids lies between 0.04 and 0.45 eV in the lower region of temperature of their liquid state. A comparison of these values with the static dielectric constant shows, that the activation energy may be regarded as a pure COULOMB energy: E2 = e2/2 ε r . The characteristic distance r has the approximate value of 8.5 Å for hydrocarbons. It decreases for halogen- and nitro-derivates. Formerly it was found that the conductivity of mixtures obeys the law σM = σAC · σB1-C. This can easily be explained assuming εM = c εA + (1 — c) εB. In the case of rather different ε values or of homologuous compounds forming complexes, σ increases. This is identical with a kink in the log σ (c) -curve.


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