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Baker Campbell Hausdorf Theorem

This is usually referred to as the Zassenhaus expansion or the Baker Campbell Hausdorf theorem [11]. As an aside a symmetrized version of this expansion terminated at the Cl term results in the Feit and Fleck [12] approximate propagator. We have shown [13] that an infinite order subset of these commutators, may be resummed exactly as an interaction propagator ... [Pg.1212]

It applies for both formulations above that the expansion in principle contains an infinite number of terms. The convergence to a few lowest order terms relies on the ability to orderly separate influences of the dominant rf irradiation terms (through a suitable interaction frame) from the less dominant internal terms of the Hamiltonian. In principle, this may be overcome using the spectral theorem (or the Caley-Hamilton theorem [57]) providing a closed (i.e., exact) solution to the Baker-Campbell-Hausdorf problem with all dependencies included in n terms where n designates the dimension of the Hilbert-space matrix representation (e.g., 2 for a single spin-1/2, 4 for a two-spin-1/2 system) [58, 59]. [Pg.9]

Now, using Baker-Hausdorf-Campbell theorem, we have... [Pg.122]


See also in sourсe #XX -- [ Pg.1212 ]




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