Particle number operator

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. Let

$|\Psi\rangle_\nu=|\phi_1,\phi_2,\cdots,\phi_n\rangle_\nu$

be a Fock state, composed of single-particle states $|\phi_i\rangle$ drawn from a basis of the underlying Hilbert space of the Fock space. Given the corresponding creation and annihilation operators $a^{\dagger}(\phi_i)$ and $a(\phi_i)\,$ we define the number operator by

$\hat{N_i} \ \stackrel{\mathrm{def}}{=}\ a^{\dagger}(\phi_i)a(\phi_i)$

and we have

$\hat{N_i}|\Psi\rangle_\nu=N_i|\Psi\rangle_\nu$

where $N_i$ is the number of particles in state $|\phi_i\rangle$. The above equality can be proven by noting that

$\begin{matrix} a(\phi_i) |\phi_1,\phi_2,\cdots,\phi_{i-1},\phi_i,\phi_{i+1},\cdots,\phi_n\rangle_\nu &=& \sqrt{N_i} |\phi_1,\phi_2,\cdots,\phi_{i-1},\phi_{i+1},\cdots,\phi_n\rangle_\nu \\ a^{\dagger}(\phi_i) |\phi_1,\phi_2,\cdots,\phi_{i-1},\phi_{i+1},\cdots,\phi_n\rangle_\nu &=& \sqrt{N_i} |\phi_1,\phi_2,\cdots,\phi_{i-1},\phi_{i},\phi_{i+1},\cdots,\phi_n\rangle_\nu \end{matrix}$

then

$\begin{matrix} \hat{N_i}|\Psi\rangle_\nu = a^{\dagger}(\phi_i)a(\phi_i) |\phi_1,\phi_2,\cdots,\phi_{i-1},\phi_i,\phi_{i+1},\cdots,\phi_n\rangle_\nu &=& \sqrt{N_i} a^{\dagger}(\phi_i) |\phi_1,\phi_2,\cdots,\phi_{i-1},\phi_{i+1},\cdots,\phi_n\rangle_\nu \\ &=& \sqrt{N_i} \sqrt{N_i} |\phi_1,\phi_2,\cdots,\phi_{i-1},\phi_{i},\phi_{i+1},\cdots,\phi_n\rangle_\nu \\&=& N_i|\Psi\rangle_\nu\\ \end{matrix}$

See also

• Harmonic oscillator
• Quantum harmonic oscillator
• Second quantization
• Quantum field theory
• Thermodynamics
• Fermion number operator

References

• Bruus, Henrik, Flensberg, Karsten. (2004). Many-body Quantum Theory in Condensed Matter Physics: An Introduction. Oxford University Press. ISBN 0-19-856633-6.
• Second quantization notes by Fradkin