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In [[quantum mechanics]], for systems where the total [[Particle number|number of particles]]
In [[quantum mechanics]], for systems where the total [[Particle number|number of particles]] may not be preserved, the '''number operator''' is the [[observable]] that counts the number of particles.

<math>|\Psi\rangle_\nu</math>composed of single-particle [[Basis (linear algebra)|basis state]]s <math>|\phi_i\rangle</math>:
The number operator acts on [[Fock space]]. Given a [[Fock state]] <math>|\Psi\rangle_\nu</math>composed of single-particle [[Basis (linear algebra)|basis state]]s <math>|\phi_i\rangle</math>:


:<math>|\Psi\rangle_\nu=|\phi_1,\phi_2,\cdots,\phi_n\rangle_\nu</math>
:<math>|\Psi\rangle_\nu=|\phi_1,\phi_2,\cdots,\phi_n\rangle_\nu</math>

Revision as of 17:24, 25 April 2015

In quantum mechanics, for systems where the total number of particles may not be preserved, the number operator is the observable that counts the number of particles.

The number operator acts on Fock space. Given a Fock state composed of single-particle basis states :

with creation and annihilation operators and we define the number operator and we have:

where is the number of particles in state . The above equality can be proven by noting that

then

See also

References

  • Bruus, Henrik, Flensberg, Karsten. (2004). Many-body Quantum Theory in Condensed Matter Physics: An Introduction. Oxford University Press. ISBN 0-19-856633-6.{{cite book}}: CS1 maint: multiple names: authors list (link)
  • Second quantization notes by Fradkin