BRST Symmetry and de Rham Cohomology by Soon-Tae Hong

Author:Soon-Tae Hong
Language: eng
Format: epub
Publisher: Springer Netherlands, Dordrecht

Source

c

Bound state, partial

0.60

0.36

Rigid rotator, massless standard

0.22

0.34

Rigid rotator, massless WOC

0.22

0.34

Rigid rotator, massive standard

0.26

0.23

Rigid rotator, massive WOC

0.27

0.23

Experiment

0.67

0.27

Now, we investigate the relations between the Hamiltonian (6.90) and the Berry phases [169]. In the Berry phase approach to the SU(3) Skyrmion, the Hamiltonian takes the simple form [170]

(6.97)

where ε K is the eigenenergy in the K state, g K is the Berry charge, and are the right and the left generators of the group SO(4) ≈ SU(2) × SU(2), respectively, and is the angular momentum of the slow rotation. We recall that on S 3

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