A large fraction of the worldwide energy production is dissipated each year by friction, causing self-evident economical and environmental impact. While search for non-dissipative motion is a long-standing and still ongoing strive, practical realizations remain essentially limited to low-temperatures, with superconductors (charge transport), or superfluids (mass transport). Here we examine a different quantum mechanism which enables frictionless motion (denoted as { superflow}) of small, weakly interacting particles through narrow nanotubes. At T=0 K complete { superflow} through ideal carbon nanotubes is possible even in the presence of corrugated interface potentials, below a critical velocity vc. This is shown by analysis of the { superflowing} density fraction. The critical velocity tends to decrease when energy corrugations becomes larger, providing a quantum analog of the semi-classical relation between friction and interface energy-landscape. Moreover, partial { superflow} (quantum superposition of { superflowing} and normal state) can persist for velocities exceeding vc by two orders of magnitude, implying quantum-mechanical friction suppression, and gradual transition to the semi-classical regime. Viscous effects -possibly emerging at finite temperature are also examined from a kinematic perspective, confirming the possible persistence of ballistic transport in the low temperature limit.
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Ambrosetti et al. (2026) studied this question.
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