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Bounce-averaged diffusion coefficients due to resonant interaction of the outer radiation belt electrons with oblique chorus waves computed in a realistic magnetic field model

机译:由于在实际磁场模型中计算的外部辐射带电子与倾斜合唱波的共振相互作用所致的弹跳平均扩散系数

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We present the results of calculations of the bounce-averaged pitch angle, mixed, and momentum diffusion coefficients in a dipole and two realistic field models (the T01s model for quiet and storm conditions). We consider resonant interactions of the outer radiation belt electrons with oblique chorus waves. We demonstrate that on the dayside, the use of a realistic magnetic field versus a dipole field only makes a significant difference for small equatorial pitch angles at energies larger than E=1MeV. On the nightside, the differences between the scattering rates calculated in the Tsyganenko and dipole models can reach several orders of magnitude at various equatorial pitch angles for electrons with E0.5MeV. The most significant changes in the scattering rates computed in the realistic and dipole magnetic fields occur during the geomagnetically active conditions. On the nightside, for E0.5MeV, the diffusion coefficients calculated in the Tsyganenko field show significant scattering near the edge of the loss cone that can produce loss of electrons to the atmosphere, while in the dipole model there is no scattering at small equatorial pitch angles. Our computations in the realistic field show that resonant interactions between electrons with E1MeV and chorus waves can be an effective net loss mechanism on both the dayside and the nightside. To explain the differences in the scattering rates associated with a change in the magnetic field model, we present the contribution of various resonant harmonics to the diffusion and examine the changes in the resonance condition.
机译:我们给出了偶极子和两个实际场模型(安静和暴风雨条件下的T01s模型)的反弹平均俯仰角,混合角和动量扩散系数的计算结果。我们考虑外部辐射带电子与倾斜合唱波的共振相互作用。我们证明,在白天,在大于E = 1MeV的能量下,对于较小的赤道俯仰角,使用真实磁场与偶极子场只会产生显着差异。在夜间,对于E0.5MeV的电子,在Tsyganenko模型和偶极子模型中计算出的散射率之间的差异可以在不同的赤道俯仰角处达到几个数量级。在实际磁场和偶极磁场中计算出的散射率的最大变化发生在地磁活动条件下。在夜间,对于E0.5MeV,在Tsyganenko场中计算出的扩散系数在损耗锥边缘附近显示出明显的散射,这会产生向大气的电子损耗,而在偶极子模型中,小赤道间距没有散射角度。我们在现实领域中的计算表明,具有E1MeV的电子与合唱波之间的共振相互作用在白天和黑夜均可成为有效的净损失机制。为了解释与磁场模型的变化相关的散射速率的差异,我们介绍了各种共振谐波对扩散的贡献,并研究了共振条件的变化。

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