Abstract
We prove two simple theorems about squeezing induced by bilinear spin-spin interactions that conserve spin parity—including a vast majority of quantum spin models implemented by state-of-the-art quantum simulators. In particular we show that squeezing captures the first form of quantum correlations which are produced (1) at equilibrium, by adiabatically turning on the spin-spin interactions starting from a factorized state aligned with an external, arbitrary field; and (2) away from equilibrium, by evolving unitarily the same state with the interacting Hamiltonian.
- Received 22 June 2021
- Accepted 11 October 2021
DOI:https://doi.org/10.1103/PhysRevA.104.L040601
©2021 American Physical Society
Physics Subject Headings (PhySH)
Atomic, Molecular & OpticalQuantum Information, Science & Technology