2013
DOI: 10.1002/nbm.2942
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A calibration‐based approach to real‐time in vivo monitoring of pyruvate C1 and C2 polarization using the JCC spectral asymmetry

Abstract: A calibration-based technique for real-time measurement of pyruvate polarization by partial integral analysis of the doublet from the neighbouring J-coupled carbon is presented. In vitro calibration data relating the C2 and C1 asymmetries to the instantaneous C1 and C2 polarizations, respectively, were acquired in blood. The feasibility of using the in vitro calibration data to determine the instantaneous in vivo C1 and C2 polarizations was demonstrated in the analysis of rat kidney and pig heart spectral data… Show more

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Cited by 12 publications
(29 citation statements)
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“…We also observe intensity asymmetries in the doublet centered at 27 and 206 ppm. We attribute this asymmetry to differential polarization of the coupled 13 C nuclei, consistent with observations made previously31. While there has been much excitement for the translation of HP MRI to the clinic, the majority of hospital scanners operate at 1.5T32.…”
Section: Discussionsupporting
confidence: 88%
“…We also observe intensity asymmetries in the doublet centered at 27 and 206 ppm. We attribute this asymmetry to differential polarization of the coupled 13 C nuclei, consistent with observations made previously31. While there has been much excitement for the translation of HP MRI to the clinic, the majority of hospital scanners operate at 1.5T32.…”
Section: Discussionsupporting
confidence: 88%
“…with normalsinθ=2italicπJ(),2italicπJ2+(),ΩIΩS2 the residual strong‐coupling characteristic of the J ‐coupling interaction between the C 1 and C 2 carbons. For [1,2‐ 13 C]Pyr, using J = 64 Hz and ( Ω I – Ω S )/2 π = 1152 Hz at 3 T and 25°C, the asymmetry parameter at thermal equilibrium is a C eq = sin θ = 0.056, as reported earlier …”
Section: Experimental Methods and Theorysupporting
confidence: 66%
“…Zero‐order and first‐order phase correction was performed on the spectra, and the metabolite time courses were calculated by integrating the [1,2‐ 13 C]Pyr doublet peaks in absorption mode. Flip angle correction was applied to the integrated data, and the time evolution of the asymmetry parameter for the C 1 and C 2 doublet was computed using the definition a C = (inner peak − outer peak)/(inner peak + outer peak), as given in Reference . The center of the chemical shift between the two carbons is conventionally taken to be zero and the peaks closer to this center are considered “inner” peaks, whereas the peaks farther from the center are termed “outer”.…”
Section: Experimental Methods and Theorymentioning
confidence: 99%
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