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Lagrangian strong form

Thus the Lagrangian strong form [LSF] which is equivalent to the weak form (4.38) is given by... [Pg.147]

Each Kn in Eq. (8) has a different overall phase, which arises because a different Lagrangian can be used for each value of n. However, there is a strong constraint on these phases, which arises because the set of Kernels must form... [Pg.11]

In the PCL the strong interaction Lagrangian of vector mesons with vector and pseudoscalar mesons has the form... [Pg.292]

The next diagram (FIG. 3) also does not contribute to the partial width for the 0 — W7r° decay. In this case the Lagrangian of the strong coupling of axial-vector mesons to vector and pseudoscalar mesons is derived in a similar way and has the form (Nasriddinov, 1994)... [Pg.293]

This result is a curious and troubling one for the prospect that there can be a classical B held that has real dynamics. This would imply that non-Abelian symmetry is determined by a Lagrangian of the form ( 32 — /i, 2J, where this is automatically zero by duality. However, if this were the case, we would still have non-Abelian symmetry as a nonLagrangian symmetry. This strongly supports the possibility that the electrodynamic vacuum will continue to exhibit non-Abelian symmetries, such as squeezed states, even if we impose E3 = B3 = 0. [Pg.410]


See other pages where Lagrangian strong form is mentioned: [Pg.310]    [Pg.240]    [Pg.82]    [Pg.458]    [Pg.109]    [Pg.317]    [Pg.221]    [Pg.188]    [Pg.56]    [Pg.814]    [Pg.86]    [Pg.246]   
See also in sourсe #XX -- [ Pg.147 ]




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