Helicity is different form Spin for massless particle(photon)?

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SUMMARY

Helicity for massless particles, such as photons, is defined as the projection of spin onto the momentum direction, resulting in helicity values of ±1. For massless particles, the spin operators Sx and Sy are zero, indicating that they possess helicity rather than traditional spin. The concept of spin for massless particles is tied to the subgroup of the Lorentz group that commutes with their 4-momentum, which differs from massive particles that have a rest frame and corresponding SO(3) spin operators. In the absence of a rest frame, massless particles exhibit helicity as the only observable characteristic.

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  • Understanding of helicity and its relation to spin in quantum mechanics
  • Familiarity with the Lorentz group and its subgroups
  • Knowledge of 4-momentum and its implications for massless particles
  • Basic concepts of gauge transformations in quantum field theory
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  • Study the properties of the Lorentz group and its representations
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  • Explore the implications of massless particles in quantum mechanics
  • Investigate the mathematical formulation of helicity and its observables
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Physicists, particularly those specializing in quantum mechanics and particle physics, as well as students seeking to understand the differences between helicity and spin in massless particles.

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As we know photon's helicity are \pm1. Helicity is the projection of the spin S onto the direction of momentum, p, which is considered as Sz.
What about Sx and Sy? They are both ZERO?
 
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Is it reasonable to say that massless particles have no spin but just helicity?
 
What we mean by the spin of a particle is the subgroup of the Lorentz group that commutes with its 4-momentum (the "little group"). For a particle with mass, go to its rest frame where the 4-momentum is Pμ = (0,0,0,1) and the spin operators are the rotations in 3-space, Sx, Sy and Sz. They form SO(3).

For a massless particle there is no rest frame, so take the 4-momentum in the z-direction, kμ = (0,0,1,1), and its spin operators are the three operators that preserve kμ.

The first one is a rotation in the (x,y) plane. This is the helicity. It acts on the components of the particle's 4-potential as Ax ± iAy → ±(Ax ± iAy).

The other two are null rotations, x → x + εk and y → y + εk. These operations just add a multiple of k to the 4-potential. But this is just a gauge transformation. So helicity is the only observable part.
 
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