首页> 外文期刊>Journal of the Optical Society of America, B. Optical Physics >Velocity distribution of laser-induced atomic polarization moments in antirelaxation-coated cell and magneto-optic rotation
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Velocity distribution of laser-induced atomic polarization moments in antirelaxation-coated cell and magneto-optic rotation

机译:激光诱导的原子在反松弛涂层中的极化速度分布和磁光旋转

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It is shown with the use of the solution of the Boltzmann equation for laser pumping in a cell with antirelaxation coating that the velocity distribution of atomic polarization moments (PMs) is essentially dependent on the value of the magnetic field H. The z-velocity distribution of PMs in a low field, H approximate to 10(-4) A/m, is a Maxwellian one with a small admixture of an almost monokinetic one. At larger field the same distribution remains for longitudinal alignment, but for transverse alignment the Maxwellian part of the distribution disappears (at H similar to 1 A/m). It appears that the radial velocity distribution is also dependent on the field H. A calculation accounting for wall Maxwellization in low field gives for the pumping power needed to saturate the magneto-optic rotation a value similar to the experimentally determined value. It is shown that the known semiphenomenological theory neglecting the Maxwellization gives an acceptable description of magneto-optic rotation only for high (approximate to 1 A/m) magnetic field. (C) 2005 Optical Society of America.
机译:通过使用Boltzmann方程的解用于在具有抗松弛涂层的单元中进行激光泵浦,可以看出原子极化矩(PMs)的速度分布基本上取决于磁场H的值。z速度分布在低场中,PM大约为10(-4)A / m的PM是具有最小混合量的几乎单动力混合的Maxwellian混合气体。在较大的磁场中,纵向对准保持相同的分布,但是对于横向对准,该分布的麦克斯韦部分消失(在H处类似于1 A / m)。似乎径向速度分布也取决于磁场H。考虑到低场中的壁Maxwellization的计算给出了使磁光旋转饱和所需的泵浦功率,该值类似于实验确定的值。结果表明,仅对高(大约1 A / m)磁场,忽略麦克斯韦化的已知半现象学理论给出了可接受的磁光旋转描述。 (C)2005年美国眼镜学会。

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