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Peierls substitution : ウィキペディア英語版
Peierls substitution
The Peierls substitution method, named after the original work by R. Peierls

is a widely employed approximation for describing tightly-bound electrons in the presence of a slowly varying magnetic vector potential.

In the presence of an external vector potential \mathbf the second quantization translation operators, which form the kinetic part
of the Hamiltonian in the tight-binding framework, are simply -
\mathbf_x = \boldsymbol^\dagger_\boldsymbol_e^_y = \boldsymbol^\dagger_\boldsymbol_e^=\frac\int_m^ A_x(x,n)\textx, \quad \theta^y_=\frac\int_n^ A_y(m,y) \texty .
The number of flux quanta per plaquette \phi_ is related to the lattice curl of the phase factor,

\boldsymbol\times\theta_=\Delta_x\theta^y_-\Delta_y\theta^x_=\left(\theta^y_-\theta^y_-\theta^x_+\theta^x_\right)=


\frac\int_\cdot \text\mathbf=2\pi\frac\int \mathbf \cdot \text\mathbf=2\pi\phi_

and the total flux through the lattice is
\Phi=\Phi_0\sum_\phi_ with \Phi_0=hc/e in cgs units (and \Phi_0=2\pi in natural units).
In addition, it is related to the accumulated phase of a single particle state, |\psi\rangle=\boldsymbol_|0\rangle surrounding a plaquette:

\mathbf_y^\dagger \mathbf_x^\dagger \mathbf_y\mathbf_x|\psi\rangle=\mathbf_y^\dagger \mathbf_x^\dagger \mathbf_y |i+1,j\rangle e^_y^\dagger \mathbf_x^\dagger |i+1,j+1\rangle e^ \right)}=


\quad\quad \mathbf_y^\dagger |i,j+1\rangle e^-\theta^x_ \right)}=
|i,j\rangle e^-\theta^x_-\theta^y_ \right)}=|i,j\rangle e^{i2\pi \phi_{m,n}}

==Introduction==
Here we give a short derivation of the Peierls substitution. Although the derivation is not very rigorous it is illuminating.

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「Peierls substitution」の詳細全文を読む



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