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For ortho-hydrogen, the nuclear wavefunction and the rotational quantum number, respectively, are

  • A.antisymmetric and even
  • B.symmetric and odd
  • C.symmetric and even
  • D.antisymmetric and odd

Answer: B

For ortho-hydrogen the nuclear wavefunction is symmetric and the rotational quantum number is odd.

Protons are fermions, so the total wavefunction of H2 must change sign when the two nuclei are exchanged. In ortho-hydrogen the nuclear spins are parallel (total nuclear spin I = 1), and the three spin functions of a triplet are symmetric under exchange. The rotational part must then be antisymmetric, and rotational functions are antisymmetric under exchange only for odd J (1, 3, 5, ...).

Para-hydrogen is the opposite case: antisymmetric nuclear spin (I = 0) paired with even J. 'Antisymmetric and even' therefore describes para, not ortho, and the two mixed combinations (symmetric with even, antisymmetric with odd) would give a total wavefunction that is symmetric under exchange, which the Pauli principle forbids.

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