Charged particle decay of theSi28giant electric dipole resonance

1983 ◽  
Vol 27 (2) ◽  
pp. 470-481 ◽  
Author(s):  
R. L. Gulbranson ◽  
L. S. Cardman ◽  
A. Doron ◽  
A. Erell ◽  
K. R. Lindgren ◽  
...  
2008 ◽  
Vol 111 ◽  
pp. 012038
Author(s):  
H Akimune ◽  
Y Banshou ◽  
H Ikemizu ◽  
M Kinoshita ◽  
M Ohta ◽  
...  

2007 ◽  
Author(s):  
T. Yamagata ◽  
H. Akimune ◽  
S. Nakayama ◽  
M. Fujiwara ◽  
K. Fushimi ◽  
...  

2012 ◽  
Vol 85 (2) ◽  
Author(s):  
Andrzej Czarnecki ◽  
Marc Kamionkowski ◽  
Samuel K. Lee ◽  
Kirill Melnikov

Author(s):  
K. T. Knöpfle ◽  
H. Riedesel ◽  
K. Schindler ◽  
G. J. Wagner ◽  
C. Mayer-Bbricke ◽  
...  

2016 ◽  
Vol 40 ◽  
pp. 1660099 ◽  
Author(s):  
Stanislav Chekmenev

An experimental method which is aimed to find a permanent EDM of a charged particle was proposed by the JEDI (Jülich Electric Dipole moment Investigations) collaboration. EDMs can be observed by their influence on spin motion. The only possible way to perform a direct measurement is to use a storage ring. For this purpose, it was decided to carry out the first precursor experiment at the Cooler Synchrotron (COSY). Since the EDM of a particle violates CP invariance it is expected to be tiny, treatment of all various sources of systematic errors should be done with a great level of precision. One should clearly understand how misalignments of the magnets affects the beam and the spin motion. It is planned to use a RF Wien filter for the precusor experiment. In this paper the simulations of the systematic effects for the RF Wien filter device method will be discussed.


1987 ◽  
Vol 474 (2) ◽  
pp. 397-411 ◽  
Author(s):  
E. Kerkhove ◽  
P. Berkvens ◽  
R. Van de Vyver ◽  
H. Ferdinande ◽  
P. Van Otten ◽  
...  

1965 ◽  
Vol 61 (2) ◽  
pp. 269-281 ◽  
Author(s):  
D.F. Measday ◽  
A.B. Clegg ◽  
P.S. Fisher

2004 ◽  
Vol 731 ◽  
pp. 49-56 ◽  
Author(s):  
M. Hunyadi ◽  
C. Ba¨umer ◽  
A.M. van den Berg ◽  
N. Blasi ◽  
M. Csatlo´s ◽  
...  

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