Intrinsic magnetic susceptibilities of ThPtSn and UPtSn have been determined from the analysis of magnetisation isotherms recorded in the temperature range 1.9–300 K, and in magnetic field strengths up to 5 T. ThPtSn is found to be diamagnetic. Susceptibility data of UPtSn exhibit a cusp-like behaviour in the vicinity of 35 K and Curie–Weiss law above 150 K. Microscopic properties of UPtSn have been studied by
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and
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NMR Knight shift,
K, and the spin–lattice relaxation rate
1/T1 in the paramagnetic state (
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K). The Knight shift
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versus susceptibility
χ(T) plots at temperatures
T≥150 K yield the transferred hyperfine fields of +51.6 kOe/
μB for
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nuclei, and
− 13.5 kOe/
μB for
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nuclei. Plots of
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against
χ(T) for
T<150 K exhibit a deviation from the linear behaviour indicative of crystalline field effects. The temperature dependence of the
1/T1 data of
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nuclei is consistent with a model of electronic structure possessing an energy gap
Δ=12.3 meV and can explain the reported activated resistivity. Paramagnetic impurities act as relaxation centers in ThPtSn. Rapid spin diffusion plays an important role in
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relaxation while
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nuclear spins relax directly through dipole–dipole interactions with electron spins on magnetic impurities.