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When more is less: Higher magnetic fields and their limited impact on signal-to-noise ratio per unit of acquisition time in unlocalized and single-voxel magnetic resonance spectroscopy
Phys. Rev. Applied 24, 054066 – Published 21 November, 2025
DOI: https://doi.org/10.1103/j138-v9gr
Abstract
Magnetic resonance spectroscopy (MRS) offers significant diagnostic potential but is inherently constrained by a low signal-to-noise ratio (SNR). While increasing the main magnetic field strength is theoretically linked to increased SNR, practically obtained gains in SNR from to , depending on the domination of thermal noise at high , are not always realized. Especially in clinical settings, the maximum reachable SNR is further constrained by the total available acquisition time (TA) and the regulatory limits on maximum tolerable specific absorption rate (SAR). This work attempts to derive mathematical expressions that enable systematic analysis of the theoretically achievable SNR gain. One important notion in this context is the SNR gain per unit of measurement time as a function of the main magnetic field strengths in the case of unlocalized X-nuclei and localized (1H and X-nuclei) single-voxel spectroscopy (SVS) pulse sequences. Our findings indicate that, under given fixed total amount of (patient acceptable) measurement time TA and maximum tolerable SAR limitation, together with conditions that ensure the adiabaticity of specific sequences, there exists an optimal magnetic field strength that maximizes SNR per unit of measurement time (). Beyond this optimal , further increases in field strength do not yield proportional improvements in . Key factors are identified, including rf-pulse bandwidth scaling with and longitudinal relaxation time () dependencies, that impact the net gain as well. Our theoretical analysis emphasizes critical considerations for optimizing SNR per unit time in clinical MRS, even challenging the presumption that higher magnetic fields always yield improved SNR per unit of measurement time performance.
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