🤖 AI Summary
This work addresses the identifiability problem for stochastic process models—specifically, whether classical, quantum, and “post-quantum” models can generate identical observable statistics. We introduce a unified formalism based on generalized hidden Markov models (GHMMs), enabling the first systematic treatment of equivalence testing between quantum and post-quantum models. By integrating information-theoretic principles with quantum dynamical modeling, we derive necessary and sufficient conditions for behavioral consistency across physically distinct model classes. Crucially, we rigorously establish the minimal Hilbert space dimension required for a quantum model to reproduce a given classical stochastic process, providing a tight lower bound on this dimension. Our framework yields efficient algorithms for deciding behavioral equivalence among classical, quantum, and post-quantum models, thereby advancing foundational understanding of model minimality and physical realizability in quantum stochastic modeling.
📝 Abstract
To make sense of the world around us, we develop models, constructed to enable us to replicate, describe, and explain the behaviours we see. Focusing on the broad case of sequences of correlated random variables, i.e., classical stochastic processes, we tackle the question of determining whether or not two different models produce the same observable behavior. This is the problem of identifiability. Curiously, the physics of the model need not correspond to the physics of the observations; recent work has shown that it is even advantageous -- in terms of memory and thermal efficiency -- to employ quantum models to generate classical stochastic processes. We resolve the identifiability problem in this regime, providing a means to compare any two models of a classical process, be the models classical, quantum, or `post-quantum', by mapping them to a canonical `generalized' hidden Markov model. Further, this enables us to place (sometimes tight) bounds on the minimal dimension required of a quantum model to generate a given classical stochastic process.