4.2 Article

Hybrid quantum-classical algorithm for computing imaginary-time correlation functions

期刊

PHYSICAL REVIEW RESEARCH
卷 4, 期 2, 页码 -

出版社

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevResearch.4.023219

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资金

  1. JSPS KAKENHI [18H01158, 21H01041, 21H01003]
  2. JST PRESTO, Japan [JPMJPR191A, JPMJPR2012]
  3. MEXT Quantum Leap Flagship Program (MEXT QLEAP) [JPMXS0118067394, JPMXS0120319794]
  4. JST COI-NEXT program JP-MJPF2014

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This study presents a quantum-classical hybrid algorithm for computing imaginary-time Green's functions on quantum devices. By applying variational quantum simulation and a quantum circuit simulator, researchers have successfully computed the Green's functions of certain materials, demonstrating the feasibility of the proposed algorithm.
Quantitative descriptions of strongly correlated materials pose a considerable challenge in condensed matter physics and chemistry. A promising approach to address this problem is quantum embedding methods. In particular, the dynamical mean-field theory (DMFT) maps the original system to an effective quantum impurity model comprising correlated orbitals embedded in an electron bath. The biggest bottleneck in DMFT calculations is numerically solving the quantum impurity model, i.e., computing the Green's function. Past studies have proposed theoretical methods to compute the Green's function of a quantum impurity model in polynomial time using a quantum computer. So far, however, efficient methods for computing the imaginary-time Green's functions have not been established despite the advantages of the imaginary-time formulation. We propose a quantum-classical hybrid algorithm for computing imaginary-time Green's functions on quantum devices with limited hardware resources by applying the variational quantum simulation. Using a quantum circuit simulator, we verified this algorithm by computing Green's functions for a dimer model as well as a four-site impurity model obtained by DMFT calculations of the single-band Hubbard model, although our method can be applied to general imaginary-time correlation functions.

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