You signed in with another tab or window. Reload to refresh your session.You signed out in another tab or window. Reload to refresh your session.You switched accounts on another tab or window. Reload to refresh your session.Dismiss alert
The $n$-body reduced density matrix ($n$-RDM) characterizes higher order correlations in a many-body system. This quantity can be used to compute any $n$-body observable without direct access to the full wavefunction, and is experimentally measurable. Analytically, the problem of computing higher order density matrices becomes increasingly challenging as the number of coordinates grows. However, within the Luttinger liquid regime, bosonization provides access to correlation functions by representing them as exponentials of bosonic field operators. We outline the derivation of the exact $2$-RDM from bosonization and map it to the $J$-$V$ model of interacting spinless fermions in one dimension, where the low-energy sector can be described by Luttinger liquid theory. We demonstrate that the non-interacting limit reproduces the result predicted by Wick’s theorem and present an analytical result for density-density correlations, allowing for an investigation of the effects of a finite-size lattice. Our results demonstrate agreement with those obtained from density matrix renormalization group calculations. Finally, we discuss the application of our expression for computing the two-body lattice energy and static structure factor.
Description
This repository includes links, code, scripts, and data to generate the figures in a paper.
Requirements
To reproduce the plots of the paper, run the code in the jupyter notebook generate_figures.ipynb. This notebook has the following python packages as dependencies:
The creation of these materials was supported in part by the U.S. Department of Energy, Office of Science, Office of Basic Energy Sciences, under Award Number DE-SC0024333.
Figures
Figure 02: Interaction exponents
Figure 03: Density-density correlations
Figure 04: Two-RDM
Figure 05: Second cumulant
Figure 06: Difference between interacting and free fermion two-RDM