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Critical plasma density : ウィキペディア英語版
Electromagnetic electron wave
In plasma physics, an electromagnetic electron wave is a wave in a plasma which has a magnetic field component and in which primarily the electrons oscillate.
In an unmagnetized plasma, an electromagnetic electron wave is simply a light wave modified by the plasma. In a magnetized plasma, there are two modes perpendicular to the field, the O and X modes, and two modes parallel to the field, the R and L waves.
==Cut-off frequency and critical density==
In an unmagnetized plasma in the high frequency or low density limit, i.e. for \omega >> (4\pi n_ee^2/m_e)^
or
n_e << m_e\omega^2\,/\,4\pi e^2,
the wave speed is the speed of light in vacuum. As the density increases, the phase velocity increases and the group velocity decreases until the cut-off frequency where the light frequency is equal to the plasma frequency. This density is known as the critical density for the angular frequency ω of that wave and is given by
:n_c = \frac\,\omega^2.
If the critical density is exceeded, the plasma is called over-dense.
In a magnetized plasma, except for the O wave, the cut-off relationships are more complex.

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「Electromagnetic electron wave」の詳細全文を読む



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