scholarly journals Diamagnetic response of a normal-metal–superconductor proximity system at arbitrary impurity concentration

1998 ◽  
Vol 58 (21) ◽  
pp. 14531-14540 ◽  
Author(s):  
W. Belzig ◽  
C. Bruder ◽  
A. L. Fauchère
1996 ◽  
Vol 53 (9) ◽  
pp. 5727-5733 ◽  
Author(s):  
W. Belzig ◽  
C. Bruder ◽  
Gerd Schön

Author(s):  
P. J. Goodhew

Cavity nucleation and growth at grain and phase boundaries is of concern because it can lead to failure during creep and can lead to embrittlement as a result of radiation damage. Two major types of cavity are usually distinguished: The term bubble is applied to a cavity which contains gas at a pressure which is at least sufficient to support the surface tension (2g/r for a spherical bubble of radius r and surface energy g). The term void is generally applied to any cavity which contains less gas than this, but is not necessarily empty of gas. A void would therefore tend to shrink in the absence of any imposed driving force for growth, whereas a bubble would be stable or would tend to grow. It is widely considered that cavity nucleation always requires the presence of one or more gas atoms. However since it is extremely difficult to prepare experimental materials with a gas impurity concentration lower than their eventual cavity concentration there is little to be gained by debating this point.


1978 ◽  
Vol 72 (1) ◽  
pp. 125-139 ◽  
Author(s):  
J.C. Le Bosse ◽  
J. Lopez ◽  
J. Rousseau-Violet

1991 ◽  
Vol 58 (11) ◽  
pp. 1205-1207 ◽  
Author(s):  
R. H. Ono ◽  
L. F. Goodrich ◽  
J. A. Beall ◽  
M. E. Johansson ◽  
C. D. Reintsema

2021 ◽  
Vol 31 (5) ◽  
pp. 1-5
Author(s):  
Ivan P. Nevirkovets ◽  
Mikhail A. Belogolovskii ◽  
Oleg A. Mukhanov ◽  
John B. Ketterson

2021 ◽  
Vol 103 (22) ◽  
Author(s):  
Tyler R. Naibert ◽  
Hryhoriy Polshyn ◽  
Rita Garrido-Menacho ◽  
Malcolm Durkin ◽  
Brian Wolin ◽  
...  

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