1987
DOI: 10.1002/mrm.1910050303
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General solution to the NMR excitation problem for noninteracting spins

Abstract: The design of an NMR excitation scheme, whether selective or nonselective, is essentially the simultaneous inversion of an array of Bloch equations driven by magnetic fields which differ according to well-defined constraints. We find that if relaxation effects are negligible, nearly exact inversion of the Bloch equations is straightforward when performed in a special time-varying frame of reference. Repeated inversions of the Bloch equations for small perturbations provide the basis for arbitrarily large, opti… Show more

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Cited by 57 publications
(14 citation statements)
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“…One‐dimensional large‐tip‐angle RF pulse design methods have been proposed that are similar to the one we present here (12, 13). Ref 13. proposes an iterative scheme to design large‐tip‐angle pulses.…”
Section: Introductionmentioning
confidence: 86%
“…One‐dimensional large‐tip‐angle RF pulse design methods have been proposed that are similar to the one we present here (12, 13). Ref 13. proposes an iterative scheme to design large‐tip‐angle pulses.…”
Section: Introductionmentioning
confidence: 86%
“…3 but with the frequency shift correction. state, it is sufficient for the pulses to be time symmetric in the respective spin frames (17). Even though the pulse shapes we chose are universal (i.e., insensitive to the input state), it may appear that the time symmetry is lost by shifting the carrier frequency.…”
mentioning
confidence: 99%
“…The constant of proportionality k may be positive, as for ordinary pulses, negative, as for the "prefocused pulses" of Ngo and Morris (19), or zero, as for the so-called self-refocusing pulses (5,20,21). In unit of M 0 , the equilibrium magnetization value, the target function is (see Eqs.…”
Section: Linear-phase Selective 90°pulsesmentioning
confidence: 99%