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The antisymmetric tensor field carries a force that is difficult to describe in this short space.
This should moreover be (for reasons discussed earlier) an asymmetrical relation - or, more accurately, an antisymmetric relation.
That is to say, the wavefunction is antisymmetric under exchange of two particles.
For instance, the force between two quarks is attractive when both the colours and the spins of each quark are different, or (more precisely) antisymmetric .
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