How Do You Determine Rotational Invariance in a Two-Fermion System?

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To determine rotational invariance in a two-fermion system, the commutation relation [H(1), L^2] is evaluated, particularly focusing on the two-particle wave function. The ground state wave function is proposed as A (|0,1,1/2,-1/2> - |0,1,-1/2,1/2>), which yields zero when applying S1z and S2z. The angular momentum operator is defined as J^z = L_1^z + S_1^z + L_2^z + S_2^z, and to check for rotation invariance, the commutation [H^{(1)}, J^z] should be calculated. The expression for L_z is confirmed as XP_y - YP_x, but simplifying the process by directly plugging in H^{(1)} and J_z into the commutator is recommended. This approach streamlines the analysis of rotational invariance in the system.
jjohnson
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Homework Statement


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Homework Equations

The Attempt at a Solution


I suppose to determine if a hamiltonian is rotational invariant, we check if [H(1),L^2], however, I am not sure how to do it if the hamiltonian is operate on a two particle wave function.
Is it just to evaluate [S1z Z2 +S2z Z1, L1^2+L2^2]?

What is the ground state wave function for this system?
I suppose it is

A (|0,1,1/2,-1/2> - |0,1,-1/2,1/2>), if you apply S1z, you get 0. It is also true for S2z. I think I am just lost here.
 
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The rotation operator in this system will be associated with the angular momentum operator ##J^z = L_1^z + S_1^z + L_2^z + S_2^z##. To check if the perturbation alters the rotation invariant of the system, calculate the commutation ##[H^{(1)},J^z]##.
 
blue_leaf77 said:
The rotation operator in this system will be associated with the angular momentum operator ##J^z = L_1^z + S_1^z + L_2^z + S_2^z##. To check if the perturbation alters the rotation invariant of the system, calculate the commutation ##[H^{(1)},J^z]##.

Thank you fore replying.
How should I reprent ## L_z ##? is it ## XP_y - YP_x ##? Get r in spherical coordinate using raising and lowering operator and projection z axis? seems like a lot of work.
 
jjohnson said:
is it ##XP_y - YP_x## ?
Yes. ##L_z## is the orbital angular momentum of one of the fermions.
jjohnson said:
Get r in spherical coordinate using raising and lowering operator and projection z axis?
That's too much than needed. Just plug in each expression for ##H^{(1)}## and ##J_z## into the commutator ##[H^{(1)},J_z]##. It should be simple if you use the property of commutator between angular momentum and position.
 

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