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Magnetic field pseudo-vector

Two equivalent forms of Maxwell s field equations in terms of the standard vector formalism are Eq. (5), or (6) with the Lorentz gauge 9 4 = 0. The former is in terms of the antisymmetric second-rank tensor solution F, which is a combination of the electric and magnetic field variables. The latter is in terms of the vector potential, A, shown in Eq. (6) [as well as Eq. (7) in terms of the pseudo vector potential Bassuming that the parameter E, is nonzero]. (Experimental results to this point in time indicate that indeed this parameter is zero to within experimental accuracy [15]—even though the symmetry of relativity theory has no reason to exclude it. Henceforth, we will assume that this parameter is zero.)... [Pg.685]

The pseudo-spin Bloch vector of the two-level system (Haken 1981). By analogy with the Bloch vector of an electron spin interacting with an oscillating magnetic field... [Pg.517]

In Section XIII, we made a connection between the curl condition that was found to exist for Bom-Oppenheimer-Huang systems and the Yang-Mills field. Through this connection we found that the non-adiabatic coupling terms can be considered as vector potentials that have their source in pseudo magnetic... [Pg.844]


See other pages where Magnetic field pseudo-vector is mentioned: [Pg.202]    [Pg.202]    [Pg.202]    [Pg.27]    [Pg.440]    [Pg.101]    [Pg.542]    [Pg.152]   
See also in sourсe #XX -- [ Pg.202 ]




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