Inelastic-neutron-scattering measurements were performed on a single crystal of the heavy-fermion paramagnet $\mathrm{U}{\mathrm{Te}}_2$ above its superconducting temperature. We confirm the presence of antiferromagnetic fluctuations with the incommensurate wave-vector ${\mathbf{k}}_1=(0,0.57,0)$. A quasielastic signal is found, whose momentum-transfer dependence is compatible with fluctuations of magnetic moments $\mu \parallel \mathbf{a}$ with a sine-wave modulation of wave-vector ${\mathbf{k}}_1$ and in-phase moments on the nearest U atoms. Low dimensionality of the magnetic fluctuations, consequence of the ladder structure, is indicated by weak correlations along the direction $\mathbf{c}$. These fluctuations saturate below the temperature $T_1^{*}\simeq 15\mathrm{K}$, in possible relation with anomalies observed in thermodynamic, electrical-transport, and nuclear-magnetic-resonance measurements. The absence or weakness of ferromagnetic fluctuations in our data collected at temperatures down to 2.1 K and energy transfers from 0.6 to 7.5 meV is emphasized. These results constitute constraints for models of magnetically mediated superconductivity in $\mathrm{U}{\mathrm{Te}}_2$.

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• Kondo effect
• Magnetic interactions
• Magnetic susceptibility
• Magnetism
• Spin fluctuations
• Superconductivity
• Heavy-fermion systems
• Low-temperature superconductors
• Inelastic neutron scattering
• Neutron scattering