loose bound electron 弱束缚电子
K-shell bound electron K壳层束缚电子
weakest bound electron potential model 弱受约束电子势模型
bound d electron 束缚电子
electron bound 束缚电子
The essence of this phenomenon is that the interaction of a bunch of electromagnetic waves and dielectric bound electron,the medium response usually associated with frequency of wave. This is reflected in the frequency dependence of the refractive index.
产生这种现象的实质是当一束电磁波与电介质的束缚电子相互作用时,介质响应通常与光波频率有关,这体现在折射率对频率的依赖关系上,此关系称之为光纤色散特性。
参考来源 - 色散补偿光纤模块的研究·2,447,543篇论文数据,部分数据来源于NoteExpress
We calculated the he atom ground-state energy using a double generalized Laguerre polynomial in the weakest bound electron potential model (WBEPM) theory.
计算了在最弱受约束电子势模型理论下使用双广义拉盖尔多项式的氦原子基态能量。
So we can think about what is our most loosely-bound electron, what's that highest energy orbital, and it's going to be the 2 p orbital, that's going to be what's highest in energy.
我们来想一想,它“束缚得最松“的电子是哪一个,能量最高的轨道是哪一个?,它就是,2,p,轨道,是能量最高的轨道。
In this paper, the problem of surge radiation and ionization of bound electron in the interaction of ultra-short laser pulse and partial ionized plasma was studied for the first time.
第一次讨论了超强超短激光与部分离化等离子体相互作用中,束缚电子的振荡辐射和电离问题。
So we can think about what is our most loosely-bound electron, what's that highest energy orbital, and it's going to be the 2 p orbital, that's going to be what's highest in energy.
我们来想一想,它“束缚得最松“的电子是哪一个,能量最高的轨道是哪一个?,它就是,2,p,轨道,是能量最高的轨道。
So here we have energy increasing on the y-axis, and you see this straight line at the bottom here is lower down on the graph, and that's the energy of a bound electron, so that's going to be a low stable energy.
这里我们看到能量沿着y轴增加,而且在这张图片上,这条直线在底部是降低的,那是一个束缚电子的能量,所以那是一个低稳态能量。
And the thing about what Schrodinger did was all he imposed on a system was the electron behaves as a wave and is bound.
薛定谔所做的,是建立在一个系统之上,电子是像波一样运动的并且是有界限的。
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