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Comparison of one-dimensional and quasi-one-dimensional Hubbard models from the variational two-electron reduced-density-matrix method

机译:一维和准一维Hubbard模型的比较   从变分双电子降密度矩阵方法

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摘要

Minimizing the energy of an $N$-electron system as a functional of atwo-electron reduced density matrix (2-RDM), constrained by necessary$N$-representability conditions (conditions for the 2-RDM to represent anensemble $N$-electron quantum system), yields a rigorous lower bound to theground-state energy in contrast to variational wavefunction methods. Wecharacterize the performance of two sets of approximate constraints,(2,2)-positivity (DQG) and approximate (2,3)-positivity (DQGT) conditions, atcapturing correlation in one-dimensional and quasi-one-dimensional (ladder)Hubbard models. We find that, while both the DQG and DQGT conditions captureboth the weak and strong correlation limits, the more stringent DQGT conditionsimprove the ground-state energies, the natural occupation numbers, the paircorrelation function, the effective hopping, and the connected (cumulant) partof the 2-RDM. We observe that the DQGT conditions are effective at capturingstrong electron correlation effects in both one- and quasi-one-dimensionallattices for both half filling and less-than-half filling.
机译:将$ N $电子系统的能量最小化为双电子降低密度矩阵(2-RDM)的功能,并受必需的$ N $可表示性条件约束(2-RDM表示可组合的$ N $-的条件电子量子系统),与变分波函数方法相比,对基态能量产生了严格的下界。我们表征了两组近似约束(2,2)-正性(DQG)和近似(2,3)-正性(DQGT)条件的性能,捕获了一维和准一维(梯形)的相关性楷模。我们发现,尽管DQG和DQGT条件都捕获了弱的和强的相关限制,但更严格的DQGT条件改善了基态能量,自然占有数,对相关函数,有效跳变和连接的(累积的)部分2-RDM。我们观察到,对于半填充和半填充以下情况,DQGT条件可有效捕获一维和准一维晶格中的强电子相关效应。

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