Rigorous proof of the Eigenstate Thermalization Hypothesis (ETH) ansatz
Establish a rigorous proof of the Eigenstate Thermalization Hypothesis (ETH) ansatz for few-body observables in quantum chaotic many-body systems: prove that, in the eigenbasis of the Hamiltonian H with eigenvalues E_j and eigenstates |E_j>, the observable matrix elements satisfy O_ij = <E_i|O|E_j> = O(E_i) δ_ij + f(E_i, E_j) r_ij, where O(E_i) and f(E_i, E_j) are smooth functions and r_ij are random variables with zero mean and unit variance.
References
The ETH ansatz conjectures that \begin{equation}\label{ETH} O_{ij}=\bra{E_i}O\ket{E_j}=O(E_i)\delta_{ij}+f(E_i,E_j)r_{ij}, \end{equation} where $E_j$ and $\ket{j}$ denote the eigenvalue and eigenstate of $H$, respectively. $O(E_i)$ and $f(E_i,E_j)$ are smooth functions of their arguments, $\delta_{ij}$ is the Kronecker Delta function, and $r_{ij}=r*_{ji}$ are random variables with a normal distribution (zero mean and unit variance). Although ETH remains a hypothesis due to the lack of rigorous proof, most aspects of the ETH have been validated through numerical simulations .
ETH: