Adiabatic state preparation of correlated wave functions with nonlinear scheduling functions and broken-symmetry wave functions
Adiabatic state preparation (ASP) can generate the correlated wave function by simulating the time evolution of wave function under the time-dependent Hamiltonian that interpolates the Fock operator and the full electronic Hamiltonian. However, ASP is inherently unsuitable for studying strongly corr...
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Published in | Communications chemistry Vol. 5; no. 1; p. 84 |
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Main Authors | , , , , |
Format | Journal Article |
Language | English |
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25.07.2022
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Abstract | Adiabatic state preparation (ASP) can generate the correlated wave function by simulating the time evolution of wave function under the time-dependent Hamiltonian that interpolates the Fock operator and the full electronic Hamiltonian. However, ASP is inherently unsuitable for studying strongly correlated systems, and furthermore practical computational conditions for ASP are unknown. In quest for the suitable computational conditions for practical applications of ASP, we performed numerical simulations of ASP in the potential energy curves of N
2
, BeH
2
, and in the
C
2
v
quasi-reaction pathway of the Be atom insertion to the H
2
molecule, examining the effect of nonlinear scheduling functions and the ASP with broken-symmetry wave functions with the
S
2
operator as the penalty term, contributing to practical applications of quantum computing to quantum chemistry. Eventually, computational guidelines to generate the correlated wave functions having the square overlap with the complete-active space self-consistent field wave function close to unity are discussed.
Adiabatic state preparation (ASP) can generate correlated wave functions for quantum chemical calculations, but is inherently unsuitable for studying strongly correlated systems. Here, the authors perform numerical simulations of ASP for the ground state wave functions of molecules with strongly correlated electrons and propose practical conditions for preparation of close-to-exact correlated wave functions. |
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AbstractList | Adiabatic state preparation (ASP) can generate the correlated wave function by simulating the time evolution of wave function under the time-dependent Hamiltonian that interpolates the Fock operator and the full electronic Hamiltonian. However, ASP is inherently unsuitable for studying strongly correlated systems, and furthermore practical computational conditions for ASP are unknown. In quest for the suitable computational conditions for practical applications of ASP, we performed numerical simulations of ASP in the potential energy curves of N
2
, BeH
2
, and in the
C
2
v
quasi-reaction pathway of the Be atom insertion to the H
2
molecule, examining the effect of nonlinear scheduling functions and the ASP with broken-symmetry wave functions with the
S
2
operator as the penalty term, contributing to practical applications of quantum computing to quantum chemistry. Eventually, computational guidelines to generate the correlated wave functions having the square overlap with the complete-active space self-consistent field wave function close to unity are discussed.
Adiabatic state preparation (ASP) can generate correlated wave functions for quantum chemical calculations, but is inherently unsuitable for studying strongly correlated systems. Here, the authors perform numerical simulations of ASP for the ground state wave functions of molecules with strongly correlated electrons and propose practical conditions for preparation of close-to-exact correlated wave functions. Adiabatic state preparation (ASP) can generate the correlated wave function by simulating the time evolution of wave function under the time-dependent Hamiltonian that interpolates the Fock operator and the full electronic Hamiltonian. However, ASP is inherently unsuitable for studying strongly correlated systems, and furthermore practical computational conditions for ASP are unknown. In quest for the suitable computational conditions for practical applications of ASP, we performed numerical simulations of ASP in the potential energy curves of N , BeH , and in the C quasi-reaction pathway of the Be atom insertion to the H molecule, examining the effect of nonlinear scheduling functions and the ASP with broken-symmetry wave functions with the S operator as the penalty term, contributing to practical applications of quantum computing to quantum chemistry. Eventually, computational guidelines to generate the correlated wave functions having the square overlap with the complete-active space self-consistent field wave function close to unity are discussed. Abstract Adiabatic state preparation (ASP) can generate the correlated wave function by simulating the time evolution of wave function under the time-dependent Hamiltonian that interpolates the Fock operator and the full electronic Hamiltonian. However, ASP is inherently unsuitable for studying strongly correlated systems, and furthermore practical computational conditions for ASP are unknown. In quest for the suitable computational conditions for practical applications of ASP, we performed numerical simulations of ASP in the potential energy curves of N 2 , BeH 2 , and in the C 2 v quasi-reaction pathway of the Be atom insertion to the H 2 molecule, examining the effect of nonlinear scheduling functions and the ASP with broken-symmetry wave functions with the S 2 operator as the penalty term, contributing to practical applications of quantum computing to quantum chemistry. Eventually, computational guidelines to generate the correlated wave functions having the square overlap with the complete-active space self-consistent field wave function close to unity are discussed. Adiabatic state preparation (ASP) can generate the correlated wave function by simulating the time evolution of wave function under the time-dependent Hamiltonian that interpolates the Fock operator and the full electronic Hamiltonian. However, ASP is inherently unsuitable for studying strongly correlated systems, and furthermore practical computational conditions for ASP are unknown. In quest for the suitable computational conditions for practical applications of ASP, we performed numerical simulations of ASP in the potential energy curves of N2, BeH2, and in the C2v quasi-reaction pathway of the Be atom insertion to the H2 molecule, examining the effect of nonlinear scheduling functions and the ASP with broken-symmetry wave functions with the S2 operator as the penalty term, contributing to practical applications of quantum computing to quantum chemistry. Eventually, computational guidelines to generate the correlated wave functions having the square overlap with the complete-active space self-consistent field wave function close to unity are discussed.Adiabatic state preparation (ASP) can generate correlated wave functions for quantum chemical calculations, but is inherently unsuitable for studying strongly correlated systems. Here, the authors perform numerical simulations of ASP for the ground state wave functions of molecules with strongly correlated electrons and propose practical conditions for preparation of close-to-exact correlated wave functions. Adiabatic state preparation (ASP) can generate correlated wave functions for quantum chemical calculations, but is inherently unsuitable for studying strongly correlated systems. Here, the authors perform numerical simulations of ASP for the ground state wave functions of molecules with strongly correlated electrons and propose practical conditions for preparation of close-to-exact correlated wave functions. |
ArticleNumber | 84 |
Author | Shiomi, Daisuke Toyota, Kazuo Sato, Kazunobu Takui, Takeji Sugisaki, Kenji |
Author_xml | – sequence: 1 givenname: Kenji orcidid: 0000-0002-1950-5725 surname: Sugisaki fullname: Sugisaki, Kenji email: sugisaki@osaka-cu.ac.jp organization: Department of Chemistry and Molecular Materials Science, Graduate School of Science, Osaka City University, JST PRESTO, 4-1-8 Honcho, Centre for Quantum Engineering, Research and Education (CQuERE), TCG Centres for Research and Education in Science and Technology (TCG CREST) – sequence: 2 givenname: Kazuo surname: Toyota fullname: Toyota, Kazuo organization: Department of Chemistry and Molecular Materials Science, Graduate School of Science, Osaka City University – sequence: 3 givenname: Kazunobu orcidid: 0000-0003-1274-7470 surname: Sato fullname: Sato, Kazunobu email: sato@osaka-cu.ac.jp organization: Department of Chemistry and Molecular Materials Science, Graduate School of Science, Osaka City University – sequence: 4 givenname: Daisuke orcidid: 0000-0002-7135-547X surname: Shiomi fullname: Shiomi, Daisuke organization: Department of Chemistry and Molecular Materials Science, Graduate School of Science, Osaka City University – sequence: 5 givenname: Takeji orcidid: 0000-0001-6238-5215 surname: Takui fullname: Takui, Takeji email: takui@sci.osaka-cu.ac.jp organization: Department of Chemistry and Molecular Materials Science, Graduate School of Science, Osaka City University, Research Support Department/University Research Administrator Center, University Administration Division, Osaka City University, 3-3-138 Sugimoto, Sumiyoshi-ku |
BackLink | https://www.ncbi.nlm.nih.gov/pubmed/36698020$$D View this record in MEDLINE/PubMed |
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Snippet | Adiabatic state preparation (ASP) can generate the correlated wave function by simulating the time evolution of wave function under the time-dependent... Abstract Adiabatic state preparation (ASP) can generate the correlated wave function by simulating the time evolution of wave function under the time-dependent... Adiabatic state preparation (ASP) can generate correlated wave functions for quantum chemical calculations, but is inherently unsuitable for studying strongly... |
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SubjectTerms | 639/638/563/758 639/638/563/980 Adiabatic flow Beryllium hydrides Chemistry Chemistry and Materials Science Chemistry/Food Science Circuits Computers Correlation Mathematical analysis Operators (mathematics) Potential energy Quantum chemistry Quantum computing Scheduling Self consistent fields Simulation Symmetry Time dependence Wave functions |
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Title | Adiabatic state preparation of correlated wave functions with nonlinear scheduling functions and broken-symmetry wave functions |
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