Related Experiment Video
Updated: Jun 28, 2025

Computation of Atmospheric Concentrations of Molecular Clusters from ab initio Thermochemistry
Published on: April 8, 2020
Flexible Ansatz for N-Body Perturbation Theory
Ramón Alain Miranda-Quintana1, Taewon D Kim1,2, Rugwed A Lokhande1
1Department of Chemistry and Quantum Theory Project, University of Florida, Gainesville, Florida 32603, United States.
We introduce a new Flexible Ansatz for N-body Perturbation Theory (FANPT) to solve the Schrödinger equation for complex wave functions. This method provides stable, arbitrary-order solutions, even for challenging quantum systems.
Area of Science:
- Quantum Mechanics
- Computational Chemistry
- Theoretical Physics
Background:
- Solving the Schrödinger equation is crucial for understanding quantum systems.
- Existing methods face challenges with complex wave functions and strong correlations.
- A robust perturbation theory framework is needed for arbitrary N-body systems.
Purpose of the Study:
- To develop a novel perturbation theory framework for solving the Schrödinger equation.
- To introduce the Flexible Ansatz for N-body Perturbation Theory (FANPT).
- To enable projective solutions for arbitrary wave functions.
Main Methods:
- Derivation of recursive FANPT expressions.
- Extension to arbitrary orders in the perturbation hierarchy.
- Building upon the Flexible Ansatz for N-body Configuration Interaction (FANCI).
Main Results:
- FANPT provides a framework for projective solutions of the Schrödinger equation.
- Recursive expressions for arbitrary perturbation orders are derived.
- The FANPT equations demonstrate well-behaved solutions across various conditions.
Conclusions:
- FANPT offers a stable and versatile approach for quantum mechanical calculations.
- The method is effective for static correlation-dominated and nonlinear wave functions.
- FANPT advances the computational treatment of N-body quantum systems.
Related Concept Videos
Principle of Linear Impulse and Momentum for a System of Particles
Notably, internal forces between particles, occurring in equal and opposite collinear pairs, cancel out and are not part of the equation of motion. This exclusion simplifies the...
Reduced Mass Coordinates: Isolated Two-body Problem
Angular Momentum about an Arbitrary Axis
The velocity of a mass element comprises its translational velocity and the relative velocity instigated by the body's rotation. Substituting the velocity equation into...
Equation of Motion for a Rigid Body
The combined moments generated about the center of mass of the object are equal to the rate of change of the angular momentum of the body. An external force, when applied at a different...
Angular Momentum and Principle Axes of Inertia
To put this equation into simpler terms, it can be reconfigured using rectangular coordinates. This involves choosing an alternative set of XYZ axes that are arbitrarily inclined with respect to the reference frame. The process of deriving the rectangular...
Equations of Motion: Rectangular Coordinates and Cylindrical Coordinates
When a particle moves relative to an inertial frame, the equations of motion can be expressed using rectangular components. If the motion is confined to the x-y plane, the equations having the x and y coordinates only can be used to simplify the mathematical representation.
However, when particles...

