# Chirality vs Handedness

It seems to me that the terms attributing a particle

left- or right-chiral

and

left- or right-handed

are used pretty much interchangeably. Today a colleague argued that strictly speaking this is not correct. Supposedly chirality is the physical concept and handedness is the mathematical concept. Can somebody elaborate on this and explain the difference?

In elementary particle physics, chirality just defines the transformation law of the given field under the Lorentz group. For example, Dirac spinor is composed from two 2-component spinors transforming in different ways under the Lorentz transformations, while the chirality projectors $\frac{1\pm \gamma_{5}}{2}$ projects the Dirac spinor on a space of one of these two spinors. As long as the particle which is described by the Dirac spinor is massive, chirality isn't conserved in time even in free theory. However, it is Lorentz invariant.
Handedness, or (more correctly) helicity, is the projection of total angular momentum on the direction of motion. For massive particle with spin $s$, there are $2s+1$ possible values of helicity. Massless particles can only be characterized by helicity (not by spin), which can be $h$ or $-h$. The state with helicity $-h$ is called the left-handed state, while the state with helicity $+h$ is called the right-handed state. For free theory, helicity is conserved in time, but is not Lorentz invariant, which obviously follows from the definition.
• It seems that ‘left-handed’ and ‘right-handed’ apply directly only to chirality and to the massless case of helicity (which then matches chirality) but not to the massive case of helicity (except perhaps with spin $1/2$). As ‘chirality’ is essentially just Greek for ‘handedness’ (whereas ‘helicity’ is more Greek for ‘twistedness’), why is ‘handedness’ used to mean helicity instead of chirality? – Toby Bartels Jun 3 '18 at 9:04