I'm curious about the difference in physical interpretation between open and periodic boundary conditions (OBC and PBC) although they are identical in the thermodynamic limit. For simplicity, let's consider a 1-d free fermion field theory, $$ H=-\frac{1}{2}\sum_{j}^{N} (c_j^\dagger c_{j+1}+\text{h.c.}) $$ where the lattice number is $N$ and adding $c_1^\dagger c_{N}+\text{h.c.}$ for PBC. We often perform a Fourier transform to find the ground state energy and you can see both have the same dispersion relation $\cos k$ but the wavenumber is different \begin{align*} k=\begin{cases} 2n\pi/N & (n=-N/2,\cdots N/2-1, \text{PBC}) \\ n\pi/(N+1) & (n=1,\cdots N, \text{OBC}) \end{cases} \end{align*}
The ground state energy energy $E_0$ corresponds to half-filled case and both produce the same form and value in the thermodynamic limit. \begin{align*} \frac{E_0}{N}= \begin{cases} -\frac{1}{N}\sum _{k=-N/4}^{N/4-1}\cos k \to -\frac{1}{2\pi}\int_{-\pi/2}^{\pi/2}dk \cos k = -\frac{1}{\pi}\int_{0}^{\pi/2}dk \cos k =-\frac{1}{\pi} & \text{PBC} \\ -\frac{1}{N}\sum _{k=1}^{N/2}\cos k \to -\frac{1}{\pi}\int_{0}^{\pi/2}dk \cos k =-\frac{1}{\pi} & \text{OBC} \end{cases} \end{align*} Quantum mechanically, in the case of PBC, left-movers and right-movers are occupied up to the Fermi surface but the OBC seems to only occupy one side. Even if they match at the thermodynamic limit, is it okay to consider them physically equivalent?