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Density-matrix based determination of low-energy model Hamiltonians from ab initio wavefunctions

机译:从头算波函数基于密度矩阵的低能哈密顿量模型确定

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We propose a way of obtaining effective low energy Hubbard-like model Hamiltonians from ab initio quantum Monte Carlo calculations for molecular and extended systems. The Hamiltonian parameters are fit to best match the ab initio two-body density matrices and energies of the ground and excited states, and thus we refer to the method as ab initio density matrix based downfolding. For benzene (a finite system), we find good agreement with experimentally available energy gaps without using any experimental inputs. For graphene, a two dimensional solid (extended system) with periodic boundary conditions, we find the effective on-site Hubbard U*/t to be 1.3 +/- 0.2, comparable to a recent estimate based on the constrained random phase approximation. For molecules, such parameterizations enable calculation of excited states that are usually not accessible within ground state approaches. For solids, the effective Hamiltonian enables large-scale calculations using techniques designed for lattice models. (C) 2015 AIP Publishing LLC.
机译:我们提出了一种从分子和扩展系统的从头算量子蒙特卡洛计算中获得有效的低能类哈伯德模型哈密顿量的方法。哈密​​顿量参数适合于最佳匹配从头算两体密度矩阵和基态和激发态的能量,因此我们将该方法称为基于从头算密度矩阵的向下折叠。对于苯(有限系统),我们发现在不使用任何实验输入的情况下,与实验可获得的能隙具有良好的一致性。对于具有周期性边界条件的二维固体(扩展系统)石墨烯,我们发现有效的现场Hubbard U * / t为1.3 +/- 0.2,与基于受约束的随机相位近似的最新估计相当。对于分子,这种参数化可以计算通常在基态方法中不可访问的激发态。对于固体,有效的哈密顿量可以使用为晶格模型设计的技术进行大规模计算。 (C)2015 AIP Publishing LLC。

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