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Nuclear magnetic resonance in the Earth's magnetic field was studied in an urban laboratory without shielding using a second-order low- T c SQUID (superconducting quantum interference device) gradiometer. Two different configurations were investigated, one with a prepolarization field perpendicular to the measurement field and the other one with the two fields parallel but a π/2 AC pulse applied perpendicular to them. With a prepolarization field of 10 mT and a measurement field of ∼29.1 µT, the proton signal from 15 ml tap water was obtained in a one-shot measurement with high signal-to-noise ratio, and the signal was still discernible down to a sample volume of 2–3 ml. Spin–lattice relaxation time T 1 ∼1.78 s was measured from the variation of signal magnitude on the prepolarization time. Spin–spin relaxation time T 2 was estimated to be around 0.9 s from the calculated FID signal by using a special method developed based on the principle of a lock-in amplifier.
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Dong et al. (2008) studied this question.
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