NISQ era devices suffer from a number of challenges like limited qubit connectivity, short coherence times and sizable gate error rates. Thus, quantum algorithms are desired that require shallow circuit depths and low qubit counts to take advantage of these devices. We attempt to realize this with the help of classical quantum chemical theories of canonical transformation and explicit correlation. In this work, compact ab initio Hamiltonians are generated classically through an approximate similarity transformation of the Hamiltonian with a) an explicitly correlated two-body unitary operator with generalized pair excitations that remove the Coulombic electron-electron singularities from the Hamiltonian and b) a unitary one-body operator to efficiently capture the orbital relaxation effects required for accurate description of the excited states. The resulting transcorelated Hamiltonians are able to describe both ground and excited states of molecular systems in a balanced manner. Using the fermionic-ADAPT-VQE method based on the unitary coupled cluster with singles and doubles (UCCSD) ansatz and only a minimal basis set (ANO-RCC-MB), we demonstrate that the transcorrelated Hamiltonians can produce ground state energies comparable to the much larger cc-pVTZ basis. This leads to a potential reduction in the number of required CNOT gates by more than three orders of magnitude for the chemical species studied in this work. Furthermore, using the qEOM formalism in conjunction with the transcorrelated Hamiltonian, we reduce the errors in excitation energies by an order of magnitude. The transcorrelated Hamiltonians developed here are Hermitian and contain only one- and two-body interaction terms and thus can be easily combined with any quantum algorithm for accurate electronic structure simulations.
Interpolative Separable Density-Fitting for Transcorrelated Hamiltonians
Max Planck Institute for Solid State Research(马克斯·普朗克固态研究所);Yale University(耶鲁大学);Center for Advanced Systems Understanding (CASUS)(高级系统理解中心);Helmholtz-Zentrum Dresden-Rossendorf (HZDR)(德累斯顿-罗斯多夫亥姆霍兹中心);Center for Scalable Data Analytics and Artificial Intelligence (ScaDS.AI)(可扩展数据分析与人工智能中心);TU Dresden(德累斯顿工业大学)
From Wavefunction Regularity to Eigenvector Conditioning: Accuracy--Cost Trade-offs of Quantum Algorithms for Non-Hermitian Transcorrelated Hamiltonians
Center for Advanced Systems Understanding (CASUS)(高级系统理解中心);Helmholtz-Zentrum Dresden-Rossendorf (HZDR)(德累斯顿-罗斯多夫亥姆霍兹中心);Leiden University(莱顿大学);Covestro Deutschland AG(科思创德国股份公司);Dahlem Center for Complex Quantum Systems, Freie Universität Berlin(柏林自由大学达勒姆复杂量子系统中心);Walrus Computing(鲸鱼计算公司);Institute of Artificial Intelligence, Technische Universität Dresden(德累斯顿工业大学人工智能研究所);QuSoft, HIMS & IvI, University of Amsterdam(阿姆斯特丹大学QuSoft、HIMS及IvI);Center for Scalable Data Analytics and Artificial Intelligence (ScaDS.AI) Dresden/Leipzig(德累斯顿/莱比锡可扩展数据分析与人工智能中心);Technical University Dresden(德累斯顿工业大学)
Excited States from Quasiparticle Hamiltonian Based on Density Functional Theory
Duke University(杜克大学);Department of Chemistry, Duke University(杜克大学化学系);Department of Chemistry and Department of Physics, Duke University(杜克大学化学系和物理系)
Equation-of-Motion Coupled-Cluster Theory based on the 4-component Dirac-Coulomb(-Gaunt) Hamiltonian. Energies for single electron detachment, attachment and electronically excited states
本文采用四分量相对论哈密顿量的单双耦合团簇运动方程(EOM-CCSD)理论计算了电离势(IP)、电子亲和势(EA)和激发能(EE)。在这项工作中,我们利用以前开发的双群的广义张量收缩计划,并扩展它,以进行张量收缩涉及非完全对称和奇数排名张量。几个近似的自旋自由和两个组件的哈密顿量也可以在此实现中访问。我们已经将这种方法应用于卤素一氧化物(XO,X= Cl,Br,I,At,Ts)物种,以评估其他一些最近的EOMCC实现的质量,其中自旋-轨道耦合的贡献已近似在不同程度上。此外,我们还研究了CH $_2$ IBr,CH $_2$ I $_2$和I $_2^-$的各种激发态(以及同种的单电子附着和脱离电子态),并与一种密切相关的多参考耦合团簇方法,即中间哈密顿Fock空间耦合团簇单、双(IHFS-CCSD)理论进行了比较.
Efficient and reliable modeling of large $π$-electron systems with the Pariser--Parr--Pople Hamiltonian and pCCD-based methods
Institute of Physics, Faculty of Physics, Astronomy, and Informatics, Nicolaus Copernicus University in Toruń(托伦尼古拉·哥白尼大学物理、天文学与信息学学院物理研究所);Freie Universität in Berlin(柏林自由大学)
Qumode-Based Variational Quantum Eigensolver for Molecular Excited States
Yale University(耶鲁大学);University of Connecticut(康涅狄格大学);Mirion Technologies (Canberra) Inc.(米尔尼昂技术(堪培拉)公司);The University of Chicago(芝加哥大学);Yale Quantum Institute, Yale University(耶鲁大学量子研究所)