Spin vs. Helicity: Transformation under Poincare Group

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SUMMARY

This discussion focuses on the transformation of spin and helicity states under the Poincaré group, specifically through rotations around the z and x axes. Two particles are analyzed: a massive particle with a momentum-spin state and a photon with a momentum-helicity state. The transformations are expressed mathematically, demonstrating how the states change under specified rotations, with helicity being identified as Lorentz invariant. The discussion highlights the distinct treatment of spin and helicity in quantum mechanics.

PREREQUISITES
  • Understanding of Poincaré group transformations
  • Familiarity with quantum mechanics concepts, specifically spin and helicity
  • Knowledge of Lorentz invariance in particle physics
  • Basic proficiency in mathematical notation used in quantum state representation
NEXT STEPS
  • Study the mathematical framework of the Poincaré group in quantum field theory
  • Explore the implications of Lorentz invariance on particle states
  • Learn about the representation of spin and helicity in different particle types
  • Investigate the role of SO(3) matrices in quantum state transformations
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Physicists, particularly those specializing in quantum mechanics and particle physics, as well as students seeking to deepen their understanding of spin and helicity transformations in the context of the Poincaré group.

paweld
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Can somenone check if my reasoning is correct. I would like to have deeper
insight into the difference between spin and helicity.

Let's consider two particles:
(1) Particle with mass m in momentum-spin state \psi=|{p_1}^\mu=(\sqrt{p^2+m^2},0,0,p); s=1,s_{z}=1 \rangle
(these informations determine the state of this particle)
(2) Photon with momentum-helicity state \phi=|p_2^\mu=(p,0,0,p); h=1\rangle

I'm interested in how above states transform under some elements of Poinacre group.
I. space rotation through angle \alpha=\pi/2 around z axis.
(1) \psi' = \exp(i \pi/2 ) |p_1^\mu=(\sqrt{p^2+m^2},0,0,p); s=1,s_{z}=1 \rangle
(2) \phi' = \exp(i \pi/2 )|p_2^\mu=(p,0,0,p); h=1\rangle
II. space rotation through angle \alpha=\pi/2 around x axis:
(1) \psi' =1/2 |p_1^\mu=(\sqrt{p^2+m^2},0,-p,0); s=1,s_{z}=1 \rangle +
+ i/\sqrt{2}|p_1^\mu=(\sqrt{p^2+m^2},0,-p,0); s=1,s_{z}=0 \rangle +
-1/2|p_1^\mu=(\sqrt{p^2+m^2},0,-p,0); s=1,s_{z}=-1 \rangle
(2) \phi' = |p_2^\mu=(p,0,-p,0), h=1\rangle
 
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Helicity is Lorentz invariant. So you just rotate three spin and momentum components with the appropriate SO(3) matrix.
 
Last edited:

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