Two-Particle System: Boson and Fermion Eigen Energies and Wave Functions

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SUMMARY

The discussion focuses on determining the lowest eigen energy and wave function for a two-particle system consisting of bosons and fermions. For bosons, the symmetric wave function is given by \(\psi (r_{1},r_{2}) = \frac{1}{\sqrt{2}}[\psi _{1} (r1)\psi _{1} (r2) + \psi _{1} (r2)\psi _{1} (r1)]\), resulting in an energy of \(2E1\). The correct normalization for the bosonic wave function is clarified to be \(1/\sqrt{n_1!*n_2!*...*N!}\). For fermions, the antisymmetric nature of the wave function must be considered, which was not fully explored in the discussion.

PREREQUISITES
  • Understanding of quantum mechanics principles, specifically wave functions and eigen energies.
  • Familiarity with the concepts of bosons and fermions in quantum statistics.
  • Knowledge of normalization techniques for many-particle wave functions.
  • Basic mathematical skills to manipulate quantum mechanical equations.
NEXT STEPS
  • Study the properties of fermionic wave functions and their antisymmetry requirements.
  • Learn about the implications of the Pauli exclusion principle on fermionic systems.
  • Explore normalization techniques for multi-particle quantum states in greater detail.
  • Investigate the role of symmetry in quantum mechanics, particularly in relation to bosons and fermions.
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Students and researchers in quantum mechanics, particularly those focusing on particle statistics, wave function normalization, and the behavior of bosonic and fermionic systems.

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Homework Statement



Assume that we have a system where the two lowest one-particle states are [tex]\psi _{1} (r)[/tex] with eigen energy E1 and [tex]\psi _{2} (r)[/tex] with eigen energy E2. What is the lowest eigen energy E and the wave function [tex]\psi (r_{1},r_{2})[/tex] for a two-particle system if

a) they are bosons
b) they are fermions



2. The attempt at a solution

a) The symmetric (boson) wave function becomes

[tex]\psi (r_{1},r_{2}) = \frac{1}{\sqrt{2}}[\psi _{1} (r1)\psi _{1} (r2) + \psi _{1} (r2)\psi _{1} (r1)] = \frac{2}{\sqrt{2}}[\psi _{1} (r1)\psi _{1} (r2)][/tex]

The energy is of course 2E1 because bosons can be in the same quantum state.

According to my book, the answer is [tex]\psi (r_{1},r_{2}) =\psi _{1} (r1)\psi _{1} (r2)[/tex] only, so before proceeding with b) I want to know what I have done wrong.
 
Last edited:
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To ensure proper normalization, the prefactor for N-body bosonic wavefunction is not 1/sqrt(N!) but 1/sqrt(n_1!*n_2!*...*N!), where n_1, n_2, ... are number of particles in state 1, state 2, ...
 
Last edited:

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