 Solution

The hard-core chain does not undergo an energetic low-temperature collapse. For allowed configurations the only finite energy is bond stretching. If $k{\sigma }^2\gg k_{B}T$, bond lengths remain near $\sigma$ and temperature mostly changes the small bond-length fluctuations, not the distribution of angular conformations. The end-to-end distance therefore fluctuates over an expanded self-avoiding-coil distribution even at low temperature, with an approximate scale $\sigma (N-1{)}^{\nu }$ and $\nu \simeq 0.588$ for sufficiently long three-dimensional chains.

For $N=10$, the scaling is qualitative and finite-chain effects matter. An equilibrated distance-versus-sweep trace is stationary, with correlated excursions; a histogram of that trace is a distinct plot, not a curve of probability density against simulation step. Neither the temperature in kelvin nor the spring constant is specified, so an exact histogram cannot be calculated. The illustrative figure compares like-for-like coil traces rather than asserting a unique numerical simulation result.