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Representability for Quantum Theory beyond Particle-Number Conservation
1The University of Chicago, Department of Chemistry and The James Franck Institute, Chicago, Illinois 60637, USA.
Physical Review Letters
|April 11, 2026
Summary
This study solves the quantum representability problem for systems lacking particle-number conservation. It introduces a hierarchy of conditions based on the polar cone, simplifying quantum calculations using two-particle reduced density matrices (2-RDMs).
Area of Science:
- Quantum mechanics
- Computational chemistry
- Quantum information theory
Background:
- Representability of two-particle reduced density matrices (2-RDMs) is crucial for quantum calculations, determining if a 2-RDM corresponds to a physical quantum state.
- Current methods often rely on the wave function or higher-order density matrices, posing computational challenges.
Purpose of the Study:
- To solve the representability problem for quantum systems without particle-number conservation.
- To develop a systematic hierarchy of representability conditions independent of higher RDMs or the wave function.
- To establish a unified framework for both particle-number-conserving and nonconserving systems.
Main Methods:
- Characterizing physically allowed 2-RDMs using the polar cone, an 'orthogonal' geometric set.
- Deriving explicit linear equations for two-body operators within the polar cone.
- Augmenting conditions with particle-number variance.
Main Results:
- A systematic hierarchy of representability conditions for 2-RDMs in systems without particle-number conservation.
- These conditions are derived from the polar cone and do not require higher RDMs or the wave function.
- A unified framework is presented for both particle-number-conserving and nonconserving systems.
Conclusions:
- The developed conditions provide a practical approach to assessing 2-RDM representability.
- This work simplifies quantum many-body calculations by focusing on 2-RDMs.
- The unified framework enhances the applicability of 2-RDM methods across different quantum systems.
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