00:01
So, here to prove the above, we have to do, let j be total angular momentum of system.
00:13
So, a scalar variable a commutes with all the angular momentarics components of angular momentum and hence that is why a comma j, this should become equals to zero.
00:29
So, in standard basis, we can see that this should becomes the determinant of n, l of m, the matrix elements of scalar observable n dash l dash m dash or a n l m are non -zero only if l dash would become equals to l and m dash become equals to m.
01:06
So, by using this, this matrix element l dash n dash l dash m dash partitioned to n, l, l, m, this should equals to the a of n dash comma l, l, g, i, i, t, m, m because it is depending on l and m.
01:34
So, let us say this as l.
01:37
So, in a subspace of e, n comma l, the 2l plus 1 dash and 2l plus 1 matrix will be a diagonal one and all elements are equal.
02:00
So, the same holds for another scalar v and hence if we suppose let the probability of getting n comma l be the projection.
02:15
So, basically this we are taking the projection, okay, that is the projection into subspace that is e of n comma l to that of the projection p of n comma l is hermitian operator then of n comma l and be p of n comma l, this should be equals to the image of this n comma l p n comma where i should be the p of n comma l...