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Formally Exact and Practically Useful Analytic Solution of Harmonium.

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We present an exact analytic solution for harmonium, applicable to all states and interaction strengths. Our novel method efficiently solves the Schrödinger equation, offering practical wave function representations.

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Area of Science:

  • Quantum Mechanics
  • Computational Chemistry
  • Atomic Physics

Background:

  • Harmonium, a fundamental model system in quantum mechanics, describes interacting electrons.
  • Solving the Schrödinger equation for harmonium, especially with strong Coulomb interactions, is computationally challenging.
  • Existing methods often rely on approximations or basis-expansion techniques, limiting accuracy and efficiency.

Purpose of the Study:

  • To develop a novel, exact analytic solution for the Schrödinger equation of harmonium.
  • To provide accurate wave function representations for both ground and excited states across arbitrary Coulomb interaction strengths.
  • To analyze the behavior of electron density and natural occupation numbers in the strong correlation limit.

Main Methods:

  • A recently developed method for solving Schrödinger equations was employed.
  • Three formally exact analytic representations of the wave function were compared.
  • The efficiency of the new method was benchmarked against basis-expansion methods.

Main Results:

  • An exact factorized form, including a noninteger power pre-exponential factor, exponential decay, and modulator function, was identified as the optimal representation for the ground state wave function.
  • Additional factors were determined to be necessary for accurately representing excited states, incorporating nodal information.
  • The proposed method demonstrated significantly higher efficiency compared to traditional basis-expansion techniques.

Conclusions:

  • The novel analytic solution provides an accurate and efficient means to describe harmonium systems.
  • The findings offer valuable insights into the physics of strong electron correlation.
  • This method advances the computational treatment of quantum systems with arbitrary interaction strengths.