Physics:Quantum Eigenstates and eigenvalues

From HandWiki

Quantum eigenstates and eigenvalues describe the states of a quantum system that yield definite results when a physical observable is measured. Each observable is represented by an operator, whose eigenvalues correspond to measurable quantities.[1]

Eigenstates of a quantum system correspond to definite measurement outcomes, with eigenvalues representing observable quantities such as energy.

Mathematical formulation

In quantum mechanics, observables are represented by operators acting on wavefunctions. An eigenstate ψ satisfies:

A^ψ=aψ

where:

  • A^ is a linear operator
  • a is the eigenvalue
  • ψ is the eigenfunction (eigenstate)

This equation means that applying the operator does not change the form of the state, only its magnitude.[2]

Physical interpretation

Eigenstates correspond to states with definite measurement outcomes:

  • Measuring observable A in eigenstate ψ yields a with certainty
  • After measurement, the system remains in that eigenstate
  • General states can be expressed as superpositions of eigenstates

This is a central postulate of quantum mechanics.[3]

Energy eigenstates

A key example is the Hamiltonian operator H^, which represents the total energy:

H^ψn=Enψn

where:

  • En are discrete energy levels
  • ψn are stationary states

These states evolve in time as:

ψn(x,t)=ψn(x)eiEnt/[4]

Orthogonality and completeness

Eigenstates of a Hermitian operator have important properties:

  • Orthogonality: ψm*ψndx=0(mn)
  • Completeness: Any wavefunction can be expressed as a sum of eigenstates

These properties allow expansion of arbitrary quantum states in a basis of eigenfunctions.[5]

Applications

Eigenstates and eigenvalues are fundamental in:

  • Atomic and molecular spectra
  • Quantum measurements
  • Quantum computing (basis states)
  • Solving Schrödinger equations

They provide the link between mathematical operators and physical observables.[6]

See also

Table of contents (185 articles)

Index

Full contents

9. Quantum optics and experiments (5) ↑ Back to index
14. Plasma and fusion physics (8) ↑ Back to index
Conceptual illustration of plasma physics in a fusion context, showing magnetically confined ionized gas in a tokamak and the collective behavior governed by electromagnetic fields and transport processes.
Conceptual illustration of plasma physics in a fusion context, showing magnetically confined ionized gas in a tokamak and the collective behavior governed by electromagnetic fields and transport processes.

References

Author: Harold Foppele