Nuclear spin states of H2
Each hydrogen molecule (H
2) consists of two hydrogen atoms linked by a covalent bond. If we neglect the small proportion of deuterium and tritium which may be present, each hydrogen atom consists of one proton and one electron. The proton has an associated magnetic moment, which is associated with the proton's spin. In the H
2 molecule, the spins of the two hydrogen nuclei (protons) couple to form a triplet state (I = 1, α
1α
2, (α
1β
2 + β
1α
2)/(2
1/2), or β
1β
2 for which M
I = 1, 0, −1 respectively — this is
orthohydrogen) or to form a singlet state (I = 0, (α
1β
2 – β
1α
2)/(2
1/2) M
I = 0 — this is
parahydrogen). The ratio between the ortho and para forms is about 3:1 at standard temperature and pressure - a reflection of the spin degeneracy ratio, but if thermal equilibrium between the two forms is established, the para form dominates at low temperatures (approx. 99.8% at 20 K
). Other molecules and functional groups containing two hydrogen atoms, such as water and methylene, also have ortho and para forms (e.g. orthowater and parawater), although their ratios differ from that of the dihydrogen molecule.