2005
DOI: 10.1002/mrm.20751
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Velocity‐selective RF pulses in MRI

Abstract: A family of velocity-selective pulses consisting of a series of RF hard pulses followed by bipolar gradients was designed. The succession of required pulses was deduced using a k-space approach within a small tip-angle approximation. Fourier transform of the desired velocity excitation determined the flip-angle series, and the corresponding position in the generalized kspace identified the bipolar-gradient first moments. Spins from any velocity class can be selected. To illustrate this approach we designed and… Show more

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Cited by 29 publications
(33 citation statements)
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“…If the transverse magnetization is spoiled following the tip-up RF pulse (by means of spoiler gradients), the resulting longitudinal magnetization will be modulated by cos(ϕ). Interestingly, while the velocity encoding effect has found extensive applications in phase contrast MRI of flow (18,20) and moving tissues (21), and in the design of flow-selective excitation (22-24) or magnetization preparation (16), its use in flow-suppressed MRI was demonstrated only recently for vascular imaging (8-11). …”
Section: Methodsmentioning
confidence: 99%
“…If the transverse magnetization is spoiled following the tip-up RF pulse (by means of spoiler gradients), the resulting longitudinal magnetization will be modulated by cos(ϕ). Interestingly, while the velocity encoding effect has found extensive applications in phase contrast MRI of flow (18,20) and moving tissues (21), and in the design of flow-selective excitation (22-24) or magnetization preparation (16), its use in flow-suppressed MRI was demonstrated only recently for vascular imaging (8-11). …”
Section: Methodsmentioning
confidence: 99%
“…The earliest version of VS excitation pulse consists of multiple rectangular RF pulses of small flip angle interleaved with bipolar gradients . This baseline design is short and easy to implement but is prone to excitation profile shifting in proportion to off‐resonance.…”
Section: Introductionmentioning
confidence: 99%
“…Under the excitation k‐space formalism, the transverse component of excited magnetization M xy ( r , v , f ) can be written as the Fourier transform of the RF B 1 field deposited on k r ‐ k v ‐ k f space, where k r , k v , and k f are reciprocal Fourier variables of spatial position r , velocity v , and off‐resonance f , respectively . M xy ( r , v , f ) = i γ M 0 0 T B 1 ( t ) e i 2 π [ k r · r + k v · v + k f f ] d t k r ( t ) = γ 2 π t T G ( s ) ds , k v ( t ) = γ 2 π t T ( t s ) G ( s ) ds , k f ( t ) = T t where γ, M 0, and T are the gyromagnetic ratio, magnetization at equilibrium, and pulse duration, respectively.…”
Section: Methodsmentioning
confidence: 99%
“…The most systematic framework for designing VS excitation pulse sequences was provided by de Rochefort et al . The excitation k‐space initially introduced for spatially selective excitation by Pauly et al was extended to include the velocity Fourier variable.…”
mentioning
confidence: 99%