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We design a thermal bath that preserves the conservation of a system’s angular momentum or allows it to fluctuate around a specified nonzero mean while maintaining a Boltzmann distribution of energy in the steady state. We demonstrate that classical particles immersed in such baths exhibit position-momentum uncertainties with a strictly positive lower bound proportional to the absolute value of the mean angular momentum. The proportionality constant, , is dimensionless and does not depend explicitly on the system’s parameters. Remarkably, while is universally bounded by unity, it attains the exact value for particles in central potentials.

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