- #1
KFC
- 488
- 4
I am reading the book by J.J.Sakurai, in chapter 3, there is a relation given as
[tex]\langle \alpha', jm|J_z A |\alpha, jm\rangle[/tex]
Here, j is the quantum number of total angular momentum, m the component along z direction, [tex]\alpha[/tex] is the third quantum number. [tex]J_z[/tex] is angular momentum operator, A is arbritary operator. Generally, [tex]J_z[/tex] is not commutate with A, but Sakurai just give the result directly as following
[tex]m\hbar\langle \alpha', jm|A|\alpha, jm\rangle[/tex]
As you see, this just like have [tex]J_z[/tex] acting on the bar and returns the [tex]m\hbar\langle \alpha', jm|[/tex]. My question is: how can [tex]J_z[/tex] acting on the bar vector?
[tex]\langle \alpha', jm|J_z A |\alpha, jm\rangle[/tex]
Here, j is the quantum number of total angular momentum, m the component along z direction, [tex]\alpha[/tex] is the third quantum number. [tex]J_z[/tex] is angular momentum operator, A is arbritary operator. Generally, [tex]J_z[/tex] is not commutate with A, but Sakurai just give the result directly as following
[tex]m\hbar\langle \alpha', jm|A|\alpha, jm\rangle[/tex]
As you see, this just like have [tex]J_z[/tex] acting on the bar and returns the [tex]m\hbar\langle \alpha', jm|[/tex]. My question is: how can [tex]J_z[/tex] acting on the bar vector?