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NMR pp 312–315Cite as

Rotating-Frame Imaging

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Abstract

The rotating-frame counterpart to (Larmor) frequency encoding in laboratory-frame imaging experiments is “nutation frequency encoding” [199]. Instead of gradients of the external magnetic field, rotating-frame imaging is based on gradients of the RF amplitude B1. That is, the effective field in the resonantly rotating frame has the form

$$ B_{1}=B_{1}\left (r\right)=B_{1}^{(0)}+G_{1}.\ r $$
((34.1))

where we have neglected the influence of local fields by spin interactions. The B1 gradient is defined by1

$$ G_{1}=\bigtriangledown B_{1} $$
((34.2))

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Notes

  1. Note that this gradient and the nabla differential operator refer to the laboratory frame, of course.

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  2. An application of this principle has already been outlined in Sect. 21.1.1 in context with the MAGROFI diffusometry method.

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© 1997 Springer-Verlag Berlin Heidelberg

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Kimmich, R. (1997). Rotating-Frame Imaging. In: NMR. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-60582-6_34

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  • DOI: https://doi.org/10.1007/978-3-642-60582-6_34

  • Publisher Name: Springer, Berlin, Heidelberg

  • Print ISBN: 978-3-642-64465-8

  • Online ISBN: 978-3-642-60582-6

  • eBook Packages: Springer Book Archive

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