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Magnetic translation : ウィキペディア英語版
Magnetic translation

Magnetic translations are naturally defined operators acting on wave function on a two-dimensional particle in a magnetic field.
According to,〔Z.Ezawa. ''Quantum Hall Effect'', 2nd ed, World Scientific. Chapter 28〕 the motion of an electron in a magnetic field on a plane is described by the following four variables: guiding center coordinates (X,Y) and the relative coordinates (R_x,R_y) .
The guiding center coordinates are independent of the relative coordinates and, when quantized, satisfy

()=-i \ell_B^2 ,

where \ell_B=\sqrt , which makes them mathematically similar to the position and momentum operators Q =q and P=-i\hbar \frac in one-dimensional quantum mechanics.
Much like acting on a wave function f(q) of a one-dimensional quantum particle by the operators e^ and e^ generate the shift of momentum or position of the particle, for the quantum particle in 2D in magnetic field one considers the magnetic translation operators

e^,

for any pair of numbers (p_x, p_y) .
The magnetic translation operators corresponding to two different pairs (p_x,p_y) and (p'_x,p'_y) do not commute.
==References==



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