PurposeTo investigate the potential effects of [1‐13C]lactate RF saturation pulses on [13C]bicarbonate detection in hyperpolarized [1‐13C]pyruvate MRI of the brain.MethodsThirteen healthy rats underwent MRI with hyperpolarized [1‐13C]pyruvate of either the brain (n = 8) or the kidneys, heart, and liver (n = 5). Dynamic, metabolite‐selective imaging was used in a cross‐over experiment in which [1‐13C]lactate was excited with either 0° or 90° flip angles. The [13C]bicarbonate SNR and apparent [1‐13C]pyruvate‐to‐[13C]bicarbonate conversion (kPB) were determined. Furthermore, simulations were performed to identify the SNR optimal flip‐angle scheme for detection of [1‐13C]lactate and [13C]bicarbonate.ResultsIn the brain, the [13C]bicarbonate SNR was 64% higher when [1‐13C]lactate was not excited (5.8 ± 1.5 vs 3.6 ± 1.3; 1.2 to 3.3–point increase; p = 0.0027). The apparent kPB decreased 25% with [1‐13C]lactate saturation (0.0047 ± 0.0008 s−1 vs 0.0034 ± 0.0006 s−1; 95% confidence interval, 0.0006–0.0019 s−1 increase; p = 0.0049). These effects were not present in the kidneys, heart, or liver. Simulations suggest that the optimal [13C]bicarbonate SNR with a TR of 1 s in the brain is obtained with [13C]bicarbonate, [1‐13C]lactate, and [1‐13C]pyruvate flip angles of 60°, 15°, and 10°, respectively.ConclusionsRadiofrequency saturation pulses on [1‐13C]lactate limit [13C]bicarbonate detection in the brain specifically, which could be due to shuttling of lactate from astrocytes to neurons. Our results have important implications for experimental design in studies in which [13C]bicarbonate detection is warranted.