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Hamiltonian systems quasi-stationary state

The SRTS sequence consists of a preparatory pulse and an arbitrary long train of the phase-coherent RF pulses of the same flip angle applied with a constant short-repetition time. As was noted above, the "short time" in this case should be interpreted as the pulse spacing T within the sequence that meets the condition T T2 Hd. The state that is established in the spin system after the time, T2, is traditionally defined as the "steady-state free precession" (SSFP), ° and includes two other states (or sub-states) quasi-stationary, that exists at times T2effective relaxation time) and stationary, that is established after the time " 3Tie after the start of the sequence.The SSFP is a very particular state which requires a specific mechanism for its description. This mechanism was devised in articles on the basis of the effective field concept and canonical transformations. Later approaches on the basis of the average-Hamiltonian theory were developed. ... [Pg.154]


See other pages where Hamiltonian systems quasi-stationary state is mentioned: [Pg.374]    [Pg.209]    [Pg.11]    [Pg.21]    [Pg.471]   
See also in sourсe #XX -- [ Pg.491 , Pg.492 ]

See also in sourсe #XX -- [ Pg.491 , Pg.492 ]




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Quasi-stationary

Quasi-stationary states

Stationary state

Stationary systems

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