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particle number operator : ウィキペディア英語版
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^(\phi_i) and a(\phi_i)\, we define the number operator by
:\hat \ \stackrel\ a^(\phi_i)a(\phi_i)
and we have
:\hat|\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
a(\phi_i) |\phi_1,\phi_2,\cdots,\phi_,\phi_i,\phi_,\cdots,\phi_n\rangle_\nu
&=& \sqrt |\phi_1,\phi_2,\cdots,\phi_,\phi_,\cdots,\phi_n\rangle_\nu \\
a^(\phi_i) |\phi_1,\phi_2,\cdots,\phi_,\phi_,\cdots,\phi_n\rangle_\nu &=& \sqrt |\phi_1,\phi_2,\cdots,\phi_,\phi_,\phi_,\cdots,\phi_n\rangle_\nu
\end
then
:\begin
\hat|\Psi\rangle_\nu = a^(\phi_i)a(\phi_i) |\phi_1,\phi_2,\cdots,\phi_,\phi_i,\phi_,\cdots,\phi_n\rangle_\nu
&=& \sqrt a^(\phi_i) |\phi_1,\phi_2,\cdots,\phi_,\phi_,\cdots,\phi_n\rangle_\nu \\ &=& \sqrt \sqrt |\phi_1,\phi_2,\cdots,\phi_,\phi_,\phi_,\cdots,\phi_n\rangle_\nu \\&=& N_i|\Psi\rangle_\nu\\
\end
==See also==

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

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
ウィキペディアで「particle number operator」の詳細全文を読む



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