Understanding the Intrinsic Parity of Quarks and Antiquarks

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SUMMARY

The discussion centers on the intrinsic parity of quarks and antiquarks, establishing that quarks have positive parity while antiquarks possess negative parity. The parity operator, represented as γ0 for Dirac particles, flips the handedness of both quarks and antiquarks, affecting their helicity and chirality. The intrinsic parity of fermions is not uniquely defined due to phase choices, but the relative parity between particles and antiparticles is clearly defined as opposite. The implications of these parity properties on the eigenvalues and wavefunctions are also explored.

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A quark and antiquark have opposite parity. The quark is customarily taken to have positive parity. I understand this to mean that Pf = f, where f is the wavefunction of the quark and Pg = -g, where g is the wavefunction of the antiquark.

Does this mean that P acting on an antiquark wavefunction flips the handedness of the particle, but won't do this for quarks? I don't think that makes sense.
 
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Doesn't it flip the handedness of both? The space parity operator for a Dirac particle is γ0.

I'm not sure which property you mean by handedness, could be either helicity or chirality. The chirality operator is γ5, which anticommutes with γ0, hence changes sign under parity. The helicity operator is ∑·p, and ∑ commutes with γ0 but p changes sign, hence the helicity changes sign under parity also.

The intrinsic parity of a fermion is not uniquely defined, there's a choice of phase involved. The relative parity of two different fermions is well defined, and as you said, the antiparticle and the particle have opposite parity.
 
Bill_K said:
Doesn't it flip the handedness of both? The space parity operator for a Dirac particle is γ0.

I'm not sure which property you mean by handedness, could be either helicity or chirality. The chirality operator is γ5, which anticommutes with γ0, hence changes sign under parity. The helicity operator is ∑·p, and ∑ commutes with γ0 but p changes sign, hence the helicity changes sign under parity also.

The intrinsic parity of a fermion is not uniquely defined, there's a choice of phase involved. The relative parity of two different fermions is well defined, and as you said, the antiparticle and the particle have opposite parity.

Thanks for the reply! If both chirality and helicity are flipped for both particle and antiparticle, then what's the consequence of them having opposite relative parity? Doesn't the +1 eigenvalue case mean that the function is left unchanged under the parity operation?
 

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