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Symmetric properties 3 isotopomers

As discussed in preceding sections, FI and have nuclear spin 5, which may have drastic consequences on the vibrational spectra of the corresponding trimeric species. In fact, the nuclear spin functions can only have A, (quartet state) and E (doublet) symmetries. Since the total wave function must be antisymmetric, Ai rovibronic states are therefore not allowed. Thus, for 7 = 0, only resonance states of A2 and E symmetries exist, with calculated states of Ai symmetry being purely mathematical states. Similarly, only -symmetric pseudobound states are allowed for 7 = 0. Indeed, even when vibronic coupling is taken into account, only A and E vibronic states have physical significance. Table XVII-XIX summarize the symmetry properties of the wave functions for H3 and its isotopomers. [Pg.605]

This property of a reduced number of coupling elements for symmetric systems is the same for all symmetrical isotopomers regardless of isotopic masses, since all have the same common symmetry property. The formation of symmetric heavy atom isotopomers, and in the isotopically scrambled... [Pg.14]


See other pages where Symmetric properties 3 isotopomers is mentioned: [Pg.610]    [Pg.718]    [Pg.91]    [Pg.1302]    [Pg.718]    [Pg.383]    [Pg.221]   
See also in sourсe #XX -- [ Pg.713 , Pg.714 , Pg.715 , Pg.716 ]




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