PIRSA:23080032

Non-Gaussian fermionic ansatzes from many-body correlation measures

APA

Herasymenko, Y. (2023). Non-Gaussian fermionic ansatzes from many-body correlation measures. Perimeter Institute. https://pirsa.org/23080032

MLA

Herasymenko, Yaroslav. Non-Gaussian fermionic ansatzes from many-body correlation measures. Perimeter Institute, Aug. 08, 2023, https://pirsa.org/23080032

BibTex

          @misc{ pirsa_PIRSA:23080032,
            doi = {10.48660/23080032},
            url = {https://pirsa.org/23080032},
            author = {Herasymenko, Yaroslav},
            keywords = {Condensed Matter},
            language = {en},
            title = {Non-Gaussian fermionic ansatzes from many-body correlation measures},
            publisher = {Perimeter Institute},
            year = {2023},
            month = {aug},
            note = {PIRSA:23080032 see, \url{https://pirsa.org}}
          }
          

Yaroslav Herasymenko Delft University of Technology

Collection
Talk Type Scientific Series

Abstract

The notorious exponential complexity of quantum problems can be avoided for systems with limited correlations. For example, states of one-dimensional systems with bounded entanglement are approximable by matrix product states. We consider fermionic systems, where correlations can be defined as deviations from Gaussian states. Heuristically, one expects a link between compact non-Gaussian ansatzes and bounded fermionic correlations. This connection, however, has not been rigorously demonstrated. Our work resolves this conceptual gap.


We focus on pure states with a fixed number of fermions. Generalizing the so-called Plücker relations, we introduce k-particle correlation measures ω_k. The vanishing of ω_k at a constant k defines a class H_k of states with limited correlations. These sets H_k are nested, ranging from Gaussian for k=1 to the full n-fermion Hilbert space H for k=n+1. States in H_{k=O(1)} can be represented using a non-Gaussian ansatz of polynomial size. Classes H_k have physical meaning, containing all truncated perturbation series around Gaussian states. We also identify non-perturbative examples of states in H_{k=O(1)}, by a numerical study of excited states in the 1D Hubbard model. Finally, we discuss the information-theoretic implications of our results for the widely used coupled-cluster ansatz.

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