Electromagnetic field requirements for a lamb-shift spin-filter polarimeter

1995 ◽  
Author(s):  
C. D. Roper ◽  
T. B. Clegg ◽  
A. J. Mendez
1977 ◽  
Vol 12 (10) ◽  
pp. 1479-1479
Author(s):  
Y. Tagishi ◽  
S. Seki ◽  
J. Sanada
Keyword(s):  

1971 ◽  
Vol 27 (9) ◽  
pp. 599-602 ◽  
Author(s):  
Gerald G. Ohlsen ◽  
J. L. McKibben ◽  
G. P. Lawrence ◽  
P. W. Keaton ◽  
D. D. Armstrong

1977 ◽  
Vol 24 (3) ◽  
pp. 1527-1529
Author(s):  
T. A. Trainor ◽  
W. B. Ingalls ◽  
H. E. Swanson ◽  
E. G. Adelberger
Keyword(s):  

1975 ◽  
Vol 14 (12) ◽  
pp. 2033-2038
Author(s):  
Yoichi Nojiri
Keyword(s):  

The energy of any system containing charged particles arises partly from its coupling to the quantized electromagnetic field; it changes on inserting the system between conducting plates, because these alter the normal modes of the field relative to free space. We calculate to order e 2 such energy shifts for a free electron and for a hydrogen atom, neglecting spin, but allowing in full for electrostatic and retardation corrections as well as for changes in the Lamb shift proper. The potential between a particle and a single plate follows as a limiting case. An appendix details the distinction between classical and quantum effects.


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