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In [[quantum mechanics]], for systems where the total [[Particle number|number of particles]] <math>|\Psi\rangle_\nu</math>composed of single-particle [[Basis (linear algebra)|basis state]]s <math>|\phi_i\rangle</math>:
In [[quantum mechanics]], the '''particle number operator''' is an operator whose eigenvalues can be interpreted as the number of particles that are in a given state.


Assume the total [[Particle number|number of particles]] <math>|\Psi\rangle_\nu</math> is composed of single-particle [[basis]] states <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>.
with [[creation and annihilation operators]] <math>a^{\dagger}(\phi_i)</math> and <math>a(\phi_i)\,</math> we define the number operator <math>\hat{N_i} \ \stackrel{\mathrm{def}}{=}\ a^{\dagger}(\phi_i)a(\phi_i)</math> and we have:

Given [[creation and annihilation operators]] <math>a^{\dagger}(\phi_i)</math> and <math>a(\phi_i)\,</math> we define the number operator <math>\hat{N_i} \ \stackrel{\mathrm{def}}{=}\ a^{\dagger}(\phi_i)a(\phi_i)</math> and we have:


:<math>\hat{N_i}|\Psi\rangle_\nu=N_i|\Psi\rangle_\nu</math>
:<math>\hat{N_i}|\Psi\rangle_\nu=N_i|\Psi\rangle_\nu</math>

Revision as of 17:15, 25 April 2015

In quantum mechanics, the particle number operator is an operator whose eigenvalues can be interpreted as the number of particles that are in a given state.

Assume the total number of particles is composed of single-particle basis states :

.

Given 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


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