薛定谔建立了一个方程并宣称：“只要你告诉我作用于电子的力，我就能告诉你它在任意时空位置的波函数行为。”
Schrodinger came up with an equation that said: "you tell me the forces acting on the electron, and I can tell you what its wave is doing at any point in space and time."
所以我们基本上对，任何一个原子都可以这么做，我们仅仅会有越来越多的波函数，因为我们将它分为越来越多的电子。
So we can do this essentially for any atom we want, we just have more and more wave functions that we're breaking it up to as we get to more and more electrons.
薛定谔建立了一个方程并宣称：“只要你告诉我作用于电子的力，我就能告诉你它在任意时空位置的波函数行为。”
Schrödinger came up with an equation that said: "You tell me the forces acting on the electron, and I can tell you what its wave is doing at any point in space and time."
但是在我们谈论那个部分之前，在理解方面，仅仅是理解，好的，它代表了粒子，它代表了电子，这就是波函数。
But before we get to that, in terms of thinking just think, OK, this is representing my particle, this is representing my electron that's what the wave function is.
实际上当我们定义电子在这个轨道，它的波函数的确是和角度有关的。
So we do, in fact, have a dependence on what the Angle is of the electron as we define it in the orbital.
因此这里的,波函数平方也等于零，如果我们说在这整个平面上,任何地方找到一个p电子的概率都是零。
So, the wave function at all of these points in this plane is equal to zero, so therefore, also the wave function squared is going to be equal to zero.
在讨论锂时，我们也可以做，完全相同的事情，但不是把它分为两个波函数，而是分为三个波函数，因为我们有3个电子。
We can do the exact same thing when we talk about lithium, but now instead of breaking it up into two wave functions, we're breaking it up into three wave functions because we have three electrons.
分子的电子波函数受到了微扰。
本文研究了存在无序及不存在无序两种情况下，一维无公度系统的电子波函数特征。
The characteristics of electron wave functions in one-dimensional incommensurate systems with or without disorder are studied.
要求反对称波函数的粒子，如电子，叫做费米子。
Particles, such as electrons, requiring antisymmetric wave functions are called fermions.
得到了电子亚带能量和波函数随自由载流子浓度的变化规律。
The rules of electron subband energies and corresponding wave functions depending upon free carrier concentration have been obtained.
分子的电子波函数受到了微扰。
寻求多原子分子的准确电子波函数主要用mo法。
The search for accurate electronic wave functions of polyatomic molecules uses mainly the MO method.
利用强束缚量子点模型，忽略杂质对于电子波函数的影响，我们还讨论了如何利用核自旋构造量子位。
By making use of the strong bound quantum dot model and neglecting the effects of impurity on electron wave function, this thesis is also reported how to use the spin of nuclear as the quantum bit.
借助激光等离子体的光学度规，严格求解了弯曲时空中的狄喇克方程，得到了强激光等离子体中的自由电子波函数。
The wave function of free electron in a strong laser plasma is obtained by solving exactly the Dirac equation in a curved space-time with optical metric for the laser plasma.
通过两种不同方法得到了任意时刻体系的状态波函数，加深了对定域电子自旋性质的掌握。
Meanwhile, we gave the state wave function in arbitrary hour by means of different methods, which made the comprehension for the spin of localized electron easier.
电子状态用波函数描述，由电子动量的概率分布，得到电子单缝衍射的强度分布。
The state of electron is described by wave function. Intensity distribution of single slit electron diffraction is derived by probability distribution of electron momentum.
当我们把波函数平方时，就等于在某处，找到一个电子的概率密度。
And when we take the wave function and square it, that's going to be equal to the probability density of finding an electron at some point in your atom.
我们从周三开始讨论这些，而且我们将要以特别地考虑，多电子原子的波函数，为开始。
We started talking about these on Wednesday, and what we're going to start with is considering specifically the wave functions for multi-electron atoms.
给出了相应的能量本征值和严格的电子波函数。
The corresponding energy eigenvalues and exact electron eigenfunctions are deduced.
波函数二阶矩的数值结果表明，绝大多数的电子态都是局域化的。
The numerical results for second moments of wave functions are shown, most states are localized ones.
当激光场为零时，该波函数自然地过渡到相对论的自由电子波函数。
When the laser field is diminshed to zero, the wave function is naturally reduced to relativistic wave function of free electron.
给出了在矩形势垒区存在电场作用时，隧穿电子波函数的形式解。
A formal solution for the wave functions of the tunneling electrons through a rectangular barrier under the electric field is given.
而且我们也可以将它，写为一个更简单的形式，它叫做电子构型，这个仅仅是这些电子波函数的。
And we can also write this in an even simpler form, which is what's called electron configuration, and this is just a shorthand notation for these electron wave functions.
在周五，我们要开始讨论，多电子原子的波函数。
So on Friday, we'll start with talking about the wave functions for the multi-electron atoms.
所以当你将它作用于波函数时，你得到的是电子的结合能，和后面的波函数。
So when you operate on the wave function, what you end up with is getting the binding energy of the electron, and the wave function back out.
我们看过波函数，我们知道解，薛定谔方程的其他部分，就是解对于原子核的电子结合能，所以我们来看一看。
We looked at the wave functions, we know the other part of solving the Schrodinger equation is to solve for the binding energy of electrons to the nucleus, so let's take a look at those.
本文在少粒子体系波函数数值解的基础上讨论了强磁场中二维电子气的二体关联函数。
The correlation function of two dimensional electron gas with the presence of a strong perpendicular magnetic field has been studied on the basis of the wave function in small system.
SQUID的量子干涉效应，将电子对波函数代入在磁场中运动的几率流密度公式，得到在D。
SQUID. Substituting the formule of the probability current density with the electron-pair wave function, this paper obtains the relation between the magnetic flux of the loop in D.
SQUID的量子干涉效应，将电子对波函数代入在磁场中运动的几率流密度公式，得到在D。
SQUID. Substituting the formule of the probability current density with the electron-pair wave function, this paper obtains the relation between the magnetic flux of the loop in D.
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