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a

The symbol aa is context-dependent. In oscillator and quantum-optics notation, aa usually denotes an annihilation operator, often written a^\hat a when hats are shown. In expansion formulas, aa can instead be an ordinary amplitude or coefficient.

For the harmonic oscillator, aa and a†a^\dagger satisfy

[a,a†]=1,[a,a^\dagger]=1,

and act on number states as

a∣n⟩=n ∣n−1⟩,a†∣n⟩=n+1 ∣n+1⟩.a\lvert n\rangle = \sqrt n\,\lvert n-1\rangle, \qquad a^\dagger\lvert n\rangle = \sqrt{n+1}\,\lvert n+1\rangle.

The number operator is

N=a†a.N=a^\dagger a.

In the standard dimensionless oscillator convention, aa is dimensionless. Its definition absorbs the oscillator length and momentum scale. Other uses of aa, such as scattering length or lattice spacing, have units of length.

  • aa as an expansion coefficient or probability amplitude.
  • aa as scattering length in low-energy scattering.
  • aa as lattice spacing in condensed matter.
  • aa as acceleration in classical-mechanics comparisons.
  • R. Shankar, Principles of Quantum Mechanics, 2nd ed., Springer, 1994.
  • M. O. Scully and M. S. Zubairy, Quantum Optics, Cambridge University Press, 1997.