2001
DOI: 10.1006/jmre.2001.2323
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Imaging the Long-Range Dipolar Field in Structured Liquid State Samples

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Cited by 50 publications
(60 citation statements)
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References 17 publications
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“…If θ = π, the magnetization after the rf pulse reduces to (8) Equations (6a) and (6b) can be combined into two second order linear differential equations in , which can be solved with diagonalization transformation. With the initial values of the magnetization just before the rf pulse taken as and , the zeroth order transverse magnetization becomes (9) The zeroth order longitudinal magnetization can be found by solving (6b) with the substitution of (9): (10) The coefficients in (9) and (10) are…”
Section: Magnetization During a Finite Rf Pulsementioning
confidence: 99%
See 1 more Smart Citation
“…If θ = π, the magnetization after the rf pulse reduces to (8) Equations (6a) and (6b) can be combined into two second order linear differential equations in , which can be solved with diagonalization transformation. With the initial values of the magnetization just before the rf pulse taken as and , the zeroth order transverse magnetization becomes (9) The zeroth order longitudinal magnetization can be found by solving (6b) with the substitution of (9): (10) The coefficients in (9) and (10) are…”
Section: Magnetization During a Finite Rf Pulsementioning
confidence: 99%
“…1. The signal produced by the sequence exhibits interesting relaxation, diffusion, and structural properties [7][8][9][10][11][12][13][14][15][16][17], and provides contrast for magnetic resonance imaging (MRI) that is fundamentally different from that by conventional techniques [18][19][20][21][22][23][24]. Nevertheless applications of such signal have been severely limited by its small amplitude in most tissues primarily due to transverse relaxation, despite the fact that some improvement can be obtained, for example, with simultaneous acquisition of multiple orders of quantum coherence [25,26].…”
Section: Introductionmentioning
confidence: 99%
“…For example, imaging sequences utilizing DDF have been devised to provide new contrast in magnetic resonance imaging applications, 7,8 to reduce linewidths in magnetic resonance spectroscopy experiments in the presence of large magnetic field inhomogeneities, [9][10][11] for functional MRI studies, 12,13 for brown adipose tissue detection, [14][15][16] and to measure temperature in vivo with high accuracy. 17,18 The main feature of DDF-based sequences is that the DDFderived signal comes primarily from pairs of nuclear spins that are separated by a "correlation distance," a user-controllable distance that can be tuned from a few micrometers to several millimeters, allowing sample structures to be probed at a microscopic scale without the loss of sensitivity.…”
Section: Introductionmentioning
confidence: 99%
“…Some of the experiments are discussed in a non-remote detection modality in Refs. [317,318,319,320,321,322,323,324,325,326,327,328,329,330,331,332,333,334,335]. Another situation that might commonly arise in remote detection experiments is when some of the carrier nucleus is bound and some is mobile, e.g., xenon in solution with some sample of interest versus free xenon gas.…”
Section: Indirect Detection With the Distant Dipolar Fieldmentioning
confidence: 99%
“…The long-range nature of iMQCs and DDF effects have made them useful probes of mesoscopic structure: e.g., as a contrast mechanism in magnetic resonance imaging [317,318,319,320,321,322,323,324,325]; in NMR multipleecho, scattering, and microscopy-type experiments [326,327,328,329,330,331,332,333]; and even in the direct mapping of the dipolar field or magnetization distribution in solution [334,335]. Some of these experiments rely on the facts that the dipolar field is active only…”
Section: Densitymentioning
confidence: 99%