Alternating and Gaussian Fermionic Isometric Tensor Network States

Isometric tensor networks in two dimensions enable efficient and accurate study of quantum many-body states, yet the effect of the isometric restriction on the represented quantum states is not fully understood. We address this question in two main contributions. First, we introduce an improved variant of isometric tensor network states (isoTNS) in two dimensions, where the isometric arrows on the columns of the network alternate between pointing upward and downward; hence the name . Second, we introduce a numerical tool—the (isoGfTNS)—that incorporates isometric constraints into the framework of Gaussian fermionic tensor network states. We demonstrate in numerous ways that alternating isoTNSs represent many-body ground states of two-dimensional quantum systems significantly better than the original isoTNSs. First, we show that the entanglement in an isoTNS is mediated along the isometric arrows and that alternating isoTNSs mediate entanglement more efficiently than conventional isoTNSs. Second, alternating isoTNSs correspond to a deeper, and thus more representative, sequential-circuit construction of depth <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"> <a:mrow> <a:mi mathvariant="script">O</a:mi> </a:mrow> <a:mo stretchy="false">(</a:mo> <a:msub> <a:mi>L</a:mi> <a:mi>x</a:mi> </a:msub> <a:mo>⋅</a:mo> <a:msub> <a:mi>L</a:mi> <a:mi>y</a:mi> </a:msub> <a:mo stretchy="false">)</a:mo> </a:math> compared to the original isoTNSs of depth <f:math xmlns:f="http://www.w3.org/1998/Math/MathML" display="inline"> <f:mrow> <f:mi mathvariant="script">O</f:mi> </f:mrow> <f:mo stretchy="false">(</f:mo> <f:msub> <f:mi>L</f:mi> <f:mi>x</f:mi> </f:msub> <f:mo>+</f:mo> <f:msub> <f:mi>L</f:mi> <f:mi>y</f:mi> </f:msub> <f:mo stretchy="false">)</f:mo> </f:math> . Third, using the Gaussian framework and gradient-based energy minimization, we provide numerical evidence of better bond-dimension scaling and variational energy of alternating isoGfTNSs for ground states of various free-fermionic models, including the Fermi surface, the band insulator, and the <k:math xmlns:k="http://www.w3.org/1998/Math/MathML" display="inline"> <k:msub> <k:mi>p</k:mi> <k:mi>x</k:mi> </k:msub> <k:mo>+</k:mo> <k:mi>i</k:mi> <k:msub> <k:mi>p</k:mi> <k:mi>y</k:mi> </k:msub> </k:math> mean-field superconductor. Finally, benchmarking on the transverse-field Ising model, we demonstrate that an alternating isoTNS provides substantially improved performance and stability relative to the original isoTNS for the ground-state search algorithm in interacting systems.

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Journal
PRX Quantum
Published
2025-09-30
DOI
https://doi.org/10.1103/8ypw-c8t4
Primary Topic
Quantum many-body systems
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article
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article

Alternating and Gaussian Fermionic Isometric Tensor Network States

Michael P. Zaletel, Sajant Anand, Zhehao Dai, Qi Yang et al.
PRX Quantum
Quantum many-body systems
article

Alternating and Gaussian Fermionic Isometric Tensor Network States

Michael P. Zaletel, Sajant Anand, Zhehao Dai, Qi Yang, Frank Pollmann, Lei Wang, Sheng-Hsuan Lin, Yantao Wu
article en

Abstract

Isometric tensor networks in two dimensions enable efficient and accurate study of quantum many-body states, yet the effect of the isometric restriction on the represented quantum states is not fully understood. We address this question in two main contributions. First, we introduce an improved variant of isometric tensor network states (isoTNS) in two dimensions, where the isometric arrows on the columns of the network alternate between pointing upward and downward; hence the name . Second, we introduce a numerical tool—the (isoGfTNS)—that incorporates isometric constraints into the framework of Gaussian fermionic tensor network states. We demonstrate in numerous ways that alternating isoTNSs represent many-body ground states of two-dimensional quantum systems significantly better than the original isoTNSs. First, we show that the entanglement in an isoTNS is mediated along the isometric arrows and that alternating isoTNSs mediate entanglement more efficiently than conventional isoTNSs. Second, alternating isoTNSs correspond to a deeper, and thus more representative, sequential-circuit construction of depth <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"> <a:mrow> <a:mi mathvariant="script">O</a:mi> </a:mrow> <a:mo stretchy="false">(</a:mo> <a:msub> <a:mi>L</a:mi> <a:mi>x</a:mi> </a:msub> <a:mo>⋅</a:mo> <a:msub> <a:mi>L</a:mi> <a:mi>y</a:mi> </a:msub> <a:mo stretchy="false">)</a:mo> </a:math> compared to the original isoTNSs of depth <f:math xmlns:f="http://www.w3.org/1998/Math/MathML" display="inline"> <f:mrow> <f:mi mathvariant="script">O</f:mi> </f:mrow> <f:mo stretchy="false">(</f:mo> <f:msub> <f:mi>L</f:mi> <f:mi>x</f:mi> </f:msub> <f:mo>+</f:mo> <f:msub> <f:mi>L</f:mi> <f:mi>y</f:mi> </f:msub> <f:mo stretchy="false">)</f:mo> </f:math> . Third, using the Gaussian framework and gradient-based energy minimization, we provide numerical evidence of better bond-dimension scaling and variational energy of alternating isoGfTNSs for ground states of various free-fermionic models, including the Fermi surface, the band insulator, and the <k:math xmlns:k="http://www.w3.org/1998/Math/MathML" display="inline"> <k:msub> <k:mi>p</k:mi> <k:mi>x</k:mi> </k:msub> <k:mo>+</k:mo> <k:mi>i</k:mi> <k:msub> <k:mi>p</k:mi> <k:mi>y</k:mi> </k:msub> </k:math> mean-field superconductor. Finally, benchmarking on the transverse-field Ising model, we demonstrate that an alternating isoTNS provides substantially improved performance and stability relative to the original isoTNS for the ground-state search algorithm in interacting systems.

PRX QuantumVol. 6(4)
Lawrence Berkeley National Laboratory (US), University of Pittsburgh (US), Chinese Academy of Sciences (CN), University of California System (US), FZU ‒ Institute of Physics of the Academy of Sciences of the Czech Republic (CZ), University of Chinese Academy of Sciences (CN), Technical University of Munich (DE)
Openalex Percentile: Top 74%
Quantum many-body systems
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