In quark potential models the hyperfine splitting of P-wave mesons is zero in
the nonrelativistic limit, a prediction strikingly confirmed by experiment in
both charmonia and bottomonia. The result, however, ignores the coupling of
bare quarkonia to meson-meson pairs. This coupling causes mass shifts among the
states and so could potentially spoil the quark model prediction. This turns
out not to be the case: in a variety of models the hyperfine splitting remains
small despite large mass shifts. This is shown to be a generic feature of
models in which the coupling involves the creation of a light quark pair with
spin-one and the quark spin wavefunctions are conserved. This talk reports on
the results of Phys. Rev. D84, 034021 (2011).Comment: 4 pages, typo corrected. Contribution to the Proceedings of the XIV
International Conference on Hadron Spectroscopy (Hadron 2011), 13-17 June
2011, Munich, German