A symmetric top molecule with moments of inertia Ix = Iy and Iz in the body-fixed axes is described by the Hamiltonian

H = \(\frac{1}{2l_x} (L^2_x+L^2_y) + \frac{1}{2l_z} L^2_z\)

If Ix = 1 and lz = \(\frac{1}{2}\), the eigenvalues for the levels with quantum numbers = 1, ml = 1 and l = 1, ml = 0 are, respectively,

1
\(\frac{3h^2}{2}\) and -h2
2
h2 and - h2
3
\(\frac{3h^2}{2}\) and h2
4
-h2 and h2
5
Question Not Attempted

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