nuclear magneton
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2007 ◽  
Vol 22 (30) ◽  
pp. 2265-2272 ◽  
Author(s):  
A. YA. BERDNIKOV ◽  
YA. A. BERDNIKOV ◽  
A. N. IVANOV ◽  
V. A. IVANOVA ◽  
A. V. NIKITCHENKO ◽  
...  

We calculate the Σ0→Λ0 transition magnetic moment μΣ0Λ0 in the effective quark model with chiral U (3) × U (3) symmetry.5 We find that the dominant contribution is proportional to the quark condensate that indicates the important role of spontaneous breaking of chiral symmetry for its formation. Our result μΣ0Λ0 = -1.62 μN, where μN is a nuclear magneton, agrees well with the experimental data [Formula: see text]. It also agrees well both quantitatively and qualitatively with the result, obtained in the QCD sum rules approach |μΣ0Λ0| = (1.60±0.30)μN,3 where the dominant contribution is proportional to the quark condensate as well.





Author(s):  
B. A. Mamyrin ◽  
N. N. Arujev ◽  
S. A. Alekseenko


1967 ◽  
Vol 156 (4) ◽  
pp. 1062-1064 ◽  
Author(s):  
J. B. Marion ◽  
H. Winkler


Nature ◽  
1967 ◽  
Vol 213 (5076) ◽  
pp. 586-586 ◽  
Author(s):  
B. W. PETLEY ◽  
K. MORRIS


1961 ◽  
Vol 123 (1) ◽  
pp. 242-254 ◽  
Author(s):  
H. S. Boyne ◽  
P. A. Franken


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