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Researchers extract mean field single particle Hamiltonians from complex fermionic wave functions. This method offers a more accurate non-interacting description, improving perturbative approaches and verifying convergence in many-body calculations.

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Area of Science:

  • Quantum Many-Body Physics
  • Computational Chemistry
  • Condensed Matter Theory

Background:

  • Extracting single-particle descriptions from many-body wave functions is crucial for understanding complex fermionic systems.
  • Existing methods like density functional theory (DFT) on lattices struggle to accurately capture kinetic energy terms.
  • A robust method is needed to bridge the gap between interacting and non-interacting descriptions.

Purpose of the Study:

  • To develop a method for extracting mean field single particle Hamiltonians from many-body wave functions.
  • To demonstrate the applicability of this method to both lattice models and atomic systems (e.g., Neon).
  • To provide an improved starting point for perturbative methods and a convergence check for numerical calculations.

Main Methods:

  • Derivation of mean field single particle Hamiltonians directly from the many-body wave function.
  • Application to lattice models of interacting fermions.
  • Testing the approach using Neon atom in an augmented correlation-consistent polarized valence double zeta (aug-cc-pvdz) basis set.

Main Results:

  • The extracted mean field Hamiltonians provide a non-interacting description that accurately includes kinetic energy terms.
  • These Hamiltonians are found to be physically closer to the investigated problem compared to traditional lattice DFT.
  • The technique successfully validates convergence of density matrix renormalization group (DMRG) calculations for interacting fermions.

Conclusions:

  • The developed method offers a more accurate extraction of mean field Hamiltonians from fermionic wave functions.
  • These improved Hamiltonians can serve as better initial guesses for perturbative calculations.
  • The technique provides a reliable tool for assessing the convergence of many-body quantum calculations.