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Optically induced Dc magnetization in a Kerr medium with dissipation

机译:光学诱导的直流磁化在带耗散的Kerr介质中

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The static magnetization induced by an elliptically polarized optical beam in a medium with dissipation is discussed for a classical and quantized optical field in a coherent state. Exact analytical formulas that describe the dc magnetization linearly and quadratically dependent on the intensity of the optical beam with the classical field are derived for crystals and nonlinear isotropic Kerr media with dissipation. For both magnetizations the hermitian operators are also defined and then used to calculate their expectation values induced by a quantized field propagating in a Kerr medium with dissipation, which in practice is represented by an isotropic medium and by crystals with symmetries $OBAR@6m2 and 6/mmm. The positive and negative role of dissipation is shown explicitly in a fully quantitative way from the exact analytical solutions. Damping of the optical wave propagating in the medium with dissipation increases the dc magnetizations. The dissipation parts of the second- and fourth-order nonlinear magneto-electric susceptibilities influencing this magnetized process decrease the dc magnetizations and even, as in the case of the nonmagnetic crystals with the symmetries 3, $OBAR@3, 32, 3m and $OBAR@3m, lead to the appearance of dc magnetization perpendicularly directed with respect to the light propagation direction. Because optically induced dc magnetizations depend on the Stokes parameters, their space derivatives are also derived for the medium with dissipation.
机译:在相干状态下讨论通过耗散的介质中的椭圆偏振光束引起的静磁化,以常规和量化的光学。对于具有经典场的光束的强度线性和二次地相比,为具有经典领域的强度而言的精确分析公式衍生用于具有耗散的晶体和非线性各向同性克尔介质。对于磁化的磁化,也定义了密封件操作员,然后用于计算由在具有耗散的KERR介质中传播的量化场引起的预期值,其在实践中由各向同性介质和具有对称的晶体来表示$ OBAR @ 6M2和6 /毫米。耗散的正面和负面作用明确地以完全定量的方式从精确的分析解决方案中明确地示出。在具有耗散的介质中传播的光波的阻尼增加了DC磁化。影响该磁化过程的第二阶和四阶非线性磁电磁敏感性的耗散部分降低了DC磁化,甚至,如同具有对称晶体的非磁性3,OBAR @ 3,32,3M和$ OBAR @ 3M,导致直流磁化的外观垂直于光传播方向。因为光学诱导的直流磁化取决于Stokes参数,所以它们的空间衍生物也用于耗散介质。

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