We investigate the thermal equilibrium properties of kinks in a classical Φ⁴ field theory in 1+1 dimensions. From large-scale Langevin simulations we identify the temperature below which a dilute-gas description of kinks is valid. The standard dilute-gas or WKB description is shown to be remarkably accurate below this temperature. At higher ``intermediate'' temperatures, where kinks still exist, this description breaks down. By introducing a double-Gaussian variational ansatz for the eigenfunctions of the statistical transfer operator for the system, we are able to study this region analytically. In particular, our predictions for the number of kinks and the correlation length are in agreement with the simulations. The double Gaussian prediction for the characteristic temperature at which the kink description ultimately breaks down is also in accord with the simulations. We also analytically calculate the internal energy and demonstrate that the peak in the specific heat near the kink characteristic temperature is indeed due to kinks. In the neighborhood of this temperautre there appears to be an intricate energy-sharing mechanism operating between nonlinear phonons and kinks.
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Alexander et al. (1993) studied this question.
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