Editing Baryon (section)

=== Parity ===
{{Main|Parity (physics)}}

If the universe were reflected in a mirror, most of the laws of physics would be identical—things would behave the same way regardless of what we call "left" and what we call "right". This concept of mirror reflection is called "[[parity (physics)|intrinsic parity]]" or simply "parity" (''P''). [[Gravity]], the [[electromagnetic force]], and the [[strong interaction]] all behave in the same way regardless of whether or not the universe is reflected in a mirror, and thus are said to [[P-symmetry|conserve parity]] (P-symmetry). However, the [[weak interaction]] does distinguish "left" from "right", a phenomenon called [[parity violation]] (P-violation).

Based on this, if the [[wavefunction]] for each particle (in more precise terms, the [[quantum field]] for each particle type) were simultaneously mirror-reversed, then the new set of wavefunctions would perfectly satisfy the laws of physics (apart from the weak interaction). It turns out that this is not quite true: for the equations to be satisfied, the wavefunctions of certain types of particles have to be multiplied by −1, in addition to being mirror-reversed. Such particle types are said to have negative or odd parity (''P''&nbsp;=&nbsp;−1, or alternatively ''P''&nbsp;=&nbsp;–), while the other particles are said to have positive or even parity (''P''&nbsp;=&nbsp;+1, or alternatively ''P''&nbsp;=&nbsp;+).

For baryons, the parity is related to the orbital angular momentum by the relation:<ref name=WongB>S.S.M. Wong (1998b)</ref>
: <math>P=(-1)^L.\ </math>

As a consequence, baryons with no orbital angular momentum (''L''&nbsp;=&nbsp;0) all have even parity (''P''&nbsp;=&nbsp;+).