In this work rapid decarboxylation of [1,2-13C]pyruvate using hydrogen peroxide was employed to obtain hyperpolarized [1-13C]acetate. 13C polarization was transferred completely and reproducibly. The application of the concept is demonstrated for detecting [1-13C]acetate and [1-13C]acetylcarnitine in the in-vivo heart.
Acetate production
By employing decarboxylation using hydrogen peroxide, [1,2-13C]pyruvate can be split yielding carbon dioxide and [1-13C]acetate (Figure 1). Due to the rapid nature of this reaction, no significant loss of 13C polarization occurs. In addition, by optimizing the pH of the solvent, the reaction can be shifted to achieve a high yield of both or one of the products.8
Hyperpolarization
A home-built multisample dynamic nuclear polarization system9 was used to dynamically polarize samples consisting of 50.8µL [1,2-13C]pyruvic acid and 13.5mM trityl, doped with 1mM Dotarem. After 90 minutes of polarization at 1.3K, the sample was dissolved in 8mL Tris buffer (pH = 12.4). An amount of 62 µL 30% hydrogen peroxide was placed in the collecting vessel for the dissolution medium, ensuring immediate mixing with the [1,2-13C]pyruvate solution. Upon dissolution, the mixture was absorbed into a 5mL syringe and transported to the scanner where it was injected at a rate of 0.1ml/s using a custom built injection system.
Magnetic resonance spectroscopy
Spectroscopic experiments were performed on a 9.4-T MR imaging system (Biospec 94/30; Bruker BioSpin, Ettlingen, Germany). A rectangular 13C surface coil with a sensitive area of 40x30 mm2 (Rapid Biomedical, Wurzburg, Germany) was placed over the thorax for signal reception. A birdcage dual 1H/13C coil (Rapid Biomedical) was used for excitation. In-vivo dynamic 13C spectra were acquired with slice selective spectroscopy using a flip angle of 20° and a repetition time of 1s (slice thickness: 10mm). Acquisitions were triggered to peak systole and end-respiration.
Three female Spargue Dawley rats weighing 330-360g were anesthetized with 4% isoflurane in a mixture of air and oxygen (4:1), endotracheal intubation was performed, and ventilation was initiated. Anesthesia was maintained by using 1-2% isoflurane. Body temperature was kept at 37–38°C by using a warm water heating system. Two 26-gauge intravenous cannulas were placed in opposite sides of the tail, one to allow injection of the dynamic nuclear polarization substrate and one for continuous glucose infusion (15 mg/kg/min).
Data processing
Resonances were fitted using the AMARES10 algorithm as implemented in the jMRUI software package 5.2.11 The [1-13C]acetate resonance was fitted and eliminated12 prior to quantification of [1-13C]acetylcarnitine and [13C]bicarbonate.
Phantom experiments
Phantom dissolutions yielded a mean liquid state polarization of 41.0±5.6% for [1-13C]pyruvate and 36.8±6.3% for [1-13C]acetate, extrapolated to the time of dissolution. The fitted T1 of [1-13C]acetate was 44±4.6s. Peaks in the spectrum were identified as [1-13C]acetate and [13C]bicarbonate (Figure 2). No peaks originating from [1,2-13C]pyruvate were observed. Concentrations of no / full conversion were determined using leftover dissolution liquid, and found to be 67+/-6mM (n=8) for pyruvate (without H2O2) and 55+/-0 mM (n=7) for acetate (with H2O2). The injected solution was neutralized by carbon dioxide released from pyruvate (pH=8.2±0.3).
In-vivo experiments
[1-13C]acetate, [1-13C]acetylcarnitine, and [13C]bicarbonate were consistently detected. Signal-time curves were fitted. Exemplary data is shown in Figure 3. The area under the curve of [1-13C]acetylcarnitine (AUCAcCar) normalized by AUCAcetate was 2.5±0.4, 3.5±0.4%, and 4.1±0.2% (mean±standard deviation, 3 repetitions). Peak SNRAcetate was 272±93 and SNRAcCar 8.9±5.3.
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