Universal properties and dynamical bosonization of strongly interacting one-dimensional anyons

We study a one-dimensional system of interacting anyons with short-range interactions under external confinement. This model, which describes anyons with zero-range $s$-wave and $p$-wave scattering interactions in the strong interaction regime, continuously interpolates between spin-polarized fermions with $p$-wave interactions and free bosons. At zero temperature, the correlation functions decay exponentially with distance, with oscillations governed by the statistics parameter. The decay rate is maximal for $p$-wave fermions and decreases monotonically as the statistics parameter approaches the bosonic limit, where it vanishes. The momentum distribution is asymmetric, a hallmark of one-dimensional anyons, and takes the form of a shifted Lorentzian with universal power-law tails, ${lim}_{k\ensuremath{\rightarrow}\ifmmode\pm\else\textpm\fi{}\ensuremath{\infty}}n(k)\ensuremath{\sim}C/{k}^{2}$. We prove analytically that, following release from a harmonic trap, the asymptotic momentum distribution converges to that of free bosons in the same trap, a phenomenon known as dynamical bosonization. We also establish the universality of the ground-state $n$-particle reduced density matrices: their natural occupations are independent of the confining potential, while the associated natural $n$-point functions for different confinements are related through a simple analytical transformation. In particular, for the one-particle reduced density matrix, we derive exact expressions for both the natural occupations and the natural orbitals at arbitrary particle number. These results extend and unify earlier partial findings for $p$-wave fermions, and they provide a clear conceptual explanation of the double degeneracy observed in their spectrum.