Vanishing spin stiffness in the spin-1/2 Heisenberg chain for any nonzero temperature

Whether at zero spin density $m=0$ and finite temperatures $T>0$ the spin stiffness of the spin-$1\mathrm{/}2$ $XXX$ chain is finite or vanishes remains an unsolved and controversial issue, as different approaches yield contradictory results. Here we provide an exact upper bound on the stiffness within a canonical ensemble at any fixed value of spin density $m$ and show that it is proportional to $m^{2}L$ in the thermodynamic limit of chain length $L\to \mathrm{\infty }$, for any finite, nonzero temperature. Moreover, we explicitly compute the stiffness at $m=0$ and confirm that it vanishes. This allows us to exactly exclude the possibility of ballistic transport within the canonical ensemble for $T>0$.