The raising and lowering operators are denoted as Land L-, respectively. The correct commutator relation between angular momentum (L) and its various components (Lx, Ly and Lz) is

1
[L2, L+] = [L2, L-] = \(\hbar \)Lz
2
[L2, L+] = [L2, L-] = \(\hbar \)Lx
3
[L2, L+] = [L2, L-] = \(\hbar \)Ly
4
[L2, L+] = [L2, L-] = 0

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