我们的朋友薛定谔告诉我们，如果你用波函数来解决，你就会知道这些概率密度看上去的样子。
Our friend Schr? Dinger told us that if you solve for the wave function, this is what the probability densities look like.
如果我们从物理意义或者,概率密度的角度来看这个问题，我们需要把波函数平方。
So again if we look at this in terms of its physical interpretation or probability density, what we need to do is square the wave function.
如果我们要讨论概率密度，这是波函数的平方。
So if we're talking about probability density that's the wave function squared.
同样，概率密度，这就是轨道的平方，波函数的平方。
So the probability again, that's just the orbital squared, the wave function squared.
同样的，我们可以把，波函数平方考虑概率密度。
So again, we can think about the probability density in terms of squaring the wave function.
这就是概率密度，但作为，把它当成是，波函数的解，让我们先倒回来一点。
So, that's probability density, but in terms of thinking about it in terms of actual solutions to the wave function, let's take a little bit of a step back here.
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.
我们可以来看一看我们讨论过的，其它一些波函数的径向概率分布。
So, we can look at other radial probability distributions of other wave functions that we talked about.
本文通过计算指出，若微扰只与时间有关，则体系的波函数可以精确求解，从而得到跃迁概率振幅的精确表达式。
It is pointed out that the wave function of system can be exactly solved if the perturbation only depends on the time, and the exact expression of transition probability amplitude can be obtained.
简要介绍了圆形无限深势阱中粒子的波函数、概率分布等特性，以及量子围栏中粒子的运动。
The wave function and probability distribution of a particle in a infinite quantum cylinder well and particle moving in a quantum corral are briefly introduced.
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.
将电子状态用波函数描述，由动量概率分布，推出电子多缝衍射强度分布。
The state of electron is described by wave function and the intensity distribution of multiple slits 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.
我们可以讨论它，波函数的平方，概率密度，或者可以考虑它的径向概率分布。
We can talk about the wave function squared, the probability density, or we can talk about the radial probability distribution.
它达到0的地方，这意味着波函数的，平方也是，如果我们看概率密度图。
So, at this place where it hits zero, 0 that means that the square of the wave function is also going to be zero, right.
它达到0的地方，这意味着波函数的，平方也是，如果我们看概率密度图。
So, at this place where it hits zero, 0 that means that the square of the wave function is also going to be zero, right.
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