In vivo hyperpolarized 13C MR spectroscopic imaging with 1H decoupling.

Application of (13)C MRS in vivo on whole body MR system has been limited due to the low static field (and consequent low signal to noise ratio-SNR) of these scanners; thus there have been few reports of (1)H decoupled (13)C MRS in vivo using a clinical MR platform. The recent development of techniques to retain highly polarized spins in solution following DNP in a solid matrix has provided a mechanism to use endogenous pre-polarized (13)C labeled substrates to study real time cellular metabolism in vivo with high SNR. In a recent in vivo hyperpolarized metabolic imaging study using (13)C pyruvate, it has been demonstrated that the line shape (signal decay) of the resonances observed are greatly affected by J(CH) coupling in addition to inhomogeneous broadening. This study demonstrates the feasibility of improving hyperpolarized (13)C metabolic imaging in vivo by incorporating (1)H decoupling on a clinical whole body 3T MR scanner. No reduction of T1 of a pre-polarized (13)C substrate ([1-(13)C] lactate) in solution was observed when (1)H decoupling was applied with WALTZ16 sequence. Narrower linewidth for the [1-(13)C] lactate resonance was observed in hyperpolarized (13)C MRSI data in vivo with (1)H decoupling.

[1]  S J Kohler,et al.  In vivo 13carbon metabolic imaging at 3T with hyperpolarized 13C‐1‐pyruvate , 2007, Magnetic resonance in medicine.

[2]  A. J. Shaka,et al.  An improved sequence for broadband decoupling: WALTZ-16 , 1983 .

[3]  J. H. Gao,et al.  Longitudinal relaxation and diffusion measurements using magnetic resonance signals from laser-hyperpolarized 129Xe nuclei. , 1997, Journal of magnetic resonance.

[4]  John M Pauly,et al.  Hyperpolarized C‐13 spectroscopic imaging of the TRAMP mouse at 3T—Initial experience , 2007, Magnetic resonance in medicine.

[5]  J. Ardenkjær-Larsen,et al.  Increase in signal-to-noise ratio of > 10,000 times in liquid-state NMR , 2003, Proceedings of the National Academy of Sciences of the United States of America.

[6]  D. Grant,et al.  Proton‐decoupled carbon‐13 relaxation in 13CH2 and 13CH3 spin systems , 1975 .

[7]  A. L. Davis,et al.  Applications of DNP-NMR for the measurement of heteronuclear T1 relaxation times. , 2007, Journal of magnetic resonance.

[8]  A. Sherry,et al.  Dipolar cross-relaxation modulates signal amplitudes in the (1)H NMR spectrum of hyperpolarized [(13)C]formate. , 2007, Journal of magnetic resonance.

[9]  Rolf Gruetter,et al.  Localized in vivo 13C NMR spectroscopy of the brain , 2003, NMR in biomedicine.

[10]  T. Inubushi,et al.  Assessment of the specific absorption rate and calibration of decoupling parameters for proton decoupled carbon-13 MR spectroscopy at 3.0 T. , 2005, European journal of radiology.

[11]  M. Thaning,et al.  Real-time metabolic imaging. , 2006, Proceedings of the National Academy of Sciences of the United States of America.

[12]  John M Pauly,et al.  Double spin-echo sequence for rapid spectroscopic imaging of hyperpolarized 13C. , 2007, Journal of magnetic resonance.

[13]  C Hawryszko,et al.  Design and evaluation of a novel dual-tuned resonator for spectroscopic imaging , 1990 .

[14]  G. C. Levy,et al.  Carbon-13 chemical shift anisotropy relaxation in organic compounds , 1975 .

[15]  Kent Harris,et al.  Clinical experience with 13C MRS in vivo , 2003, NMR in biomedicine.