我们应该可以计算出任何一个,我们想要谈论的原子的有效电荷量，只要我们知道电离能是多少。
So we should be able to calculate a z effective for any atom that we want to talk about, as long as we know what that ionization energy is.
该技术的研发团队展示了几种原子级尺寸的，采用不同的硅锗材料制成的分层结构纳米线，这种纳米线可以有效地传输电荷。
The development team demonstrated nanowires with layers of the different silicon and germanium materials that were atomically sharp and therefore more efficient at carrying electronic charges.
它们受到少的屏蔽,因为它们离原子核更近，它们感觉到一个更大的有效电荷量。
They're less shielded because they're closer to the nucleus, they feel a greater z effective.
第一个是有效核电量，或者说实际感受到的核电荷量，又或者我想我可以说就是，使它们保持在一起的,原子核的电荷量。
The first is this the z effective, or how much charge is actually in the nucleus that's felt, Z or the I guess we would say the z, how much the charge is on the nucleus that holds it close together.
电子完全抵消了来自原子核的等量电荷,这样我们仅仅看到有效的z为，在极端案例b中。
The electron completely canceled out 1 it's equivalent of charge from the nucleus, such that we only saw in a z effective of 1.
你们为什么不看一下这个然后告诉我对,于一个锂原子中的2s电子哪些是可能,的？它的有效电荷量,可能等于？
So, why don't you take a look at this and tell me which are possible for a 2 s electron in a lithium atom where z 3 is going to be equal to three?
我也想指出的一点是它们不同的方式,有效的z事实上不同于原子核的，总电荷量,因为屏蔽效应。
And the point that I also want to make is the way that they differ, z effective actually differs from the total charge in the nucleus due to an idea called shielding.
通过引入“对势函数的有效核电荷”，讨论了氩原子场的物理特征。
By introducing "the effective nucleus charge number for the potential", the physical features of argon atom field have been discussed.
通过引入“对势函数的有效核电荷”，讨论了氩原子场的物理特征。
By introducing "the effective nucleus charge number for the potential", the physical features of argon atom field have been discussed.
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