The Azimuthal Equation方位角方程
Upon separation of the Schrodinger equation for the hydrogen atom, the azimuthal equation is: 在分离氢原子的薛定谔方程后,得到极角方程为:
![]() This is the easiest of the three separated equations to solve and gives the form 这是三个分离方程中最容易求解的,给出了形式
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Index Schrodinger equation concepts Hydrogen concepts 索引 希尔伯特方程概念 氢原子概念 | ||
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The Magnetic Quantum Number磁量子数
From the azimuthal equation of the hydrogen Schrodinger equation comes a quantum number with the constraint 从氢原子的薛定谔方程的方位角方程中得出一个量子数,其有约束条件
![]() While the azimuthal dependence of the wavefunction only requires the quantum number to be an integer, the coupling to the colatitude equation further constrains that integer to be less than or equal to the orbital quantum number. The direct implication of this quantum number is that the z-component of angular momentum is quantized according to 尽管波函数的方位角依赖性仅要求量子数为整数,但与极角方程的耦合进一步将该整数限制为小于或等于轨道量子数。这个量子数的直接含义是,角动量的z分量根据下式被量子化:
![]() It is called the magnetic quantum number because the application of an external magnetic field causes a splitting of spectral lines called the Zeeman effect. The different orientations of orbital angular momentum represented by the magnetic quantum number can be visualized in terms of a vector model. 它被称为磁量子数,因为外加磁场会使谱线分裂,这种现象称为塞曼效应。磁量子数所表示的轨道角动量的不同方向可以用矢量模型来形象化。
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Index Schrodinger equation concepts Hydrogen concepts 索引 希尔伯特方程概念 氢原子概念 | ||
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Selection Rules for Electronic Transitions电子跃迁的选择规则
In spectral phenomena such as the Zeeman effect it becomes evident that transitions are not observed between all pairs of energy levels. Some transitions are "forbidden" ( i.e., highly improbable) while others are "allowed" by a set of selection rules. The number of split components observed in the Zeeman effect is consistent with the selection rules: 在诸如塞曼效应这样的谱现象中,可以看出并非所有能量级之间的跃迁都会被观察到。某些跃迁是‘被禁止的’(即极不可能发生),而另一些则根据一组选择规则被‘允许’。在塞曼效应中观察到的分裂成分数目与选择规则一致:
![]() These are the selection rules for an electric dipole transition. One can say that the oscillating electric field associated with the transitions resembles an oscillating electric dipole. When this is expressed in quantum terms, photon emission is always accompanied by a change of 1 in the orbital angular momentum quantum number. The magnetic quantum number can change by zero or one unit. 这些是电偶极跃迁的选择规则。可以说,与跃迁相关的振荡电场类似于振荡的电偶极子。当用量子术语表达时,光子发射总是伴随着轨道角动量量子数的变化为1。磁量子数可以变化0或1个单位。
Another approach to the selection rules is to note that any electron transition which involves the emission of a photon must involve a change of 1 in the angular momentum. The photon is said to have an intrinsic angular momentum or "spin" of one, so that conservation of angular momentum in photon emission requires a change of 1 in the atom's angular momentum. The electron spin quantum number does not change in such transitions, so an additional selection rule is: 另一种确定选择规则的方法是注意到任何涉及光子发射的电子跃迁都必须导致角动量的变化为1。光子具有固有的角动量或“自旋”为1,因此在光子发射过程中,角动量守恒要求原子的角动量也必须变化1。电子自旋量子数在这种跃迁中不发生变化,因此又得到一个额外的选择规则:
![]() The total angular momentum may change by either zero or one: 总角动量可能保持不变或增加一个单位:
![]() 这个最后的选择规则有一个例外,即不能从j=0过渡到j=0;即由于矢量角动量在电子跃迁中必须改变一个单位,因此j=0到j=0的跃迁是不可能的,因为没有总角动量可以重新定向以产生1的改变。 |
Index Schrodinger equation concepts Hydrogen concepts Atomic structure concepts 索引薛定谔方程概念 氢概念 原子结构概念 | ||
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