How does parity affect particle exchange in para- and ortho-hydrogen?

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SUMMARY

The discussion centers on the relationship between parity and particle exchange in para- and ortho-hydrogen. It is established that the overall wavefunction must be antisymmetric for identical particles, leading to a symmetric spatial wavefunction for para-hydrogen, which has an antisymmetric spin state. The parity of a state, defined by the angular momentum quantum number l as (-1)^l, restricts l to even values for para-hydrogen. Additionally, the concept that parity transformation resembles particle exchange is clarified, emphasizing its significance in understanding wavefunction symmetry.

PREREQUISITES
  • Understanding of quantum mechanics principles, particularly wavefunctions
  • Familiarity with the concepts of parity and angular momentum in quantum systems
  • Knowledge of antisymmetric and symmetric states in particle physics
  • Basic grasp of particle exchange and its implications in quantum statistics
NEXT STEPS
  • Explore the implications of antisymmetry in multi-particle systems
  • Study the role of parity in quantum mechanics, specifically in relation to angular momentum
  • Investigate the differences between para-hydrogen and ortho-hydrogen states
  • Learn about the mathematical representation of wavefunctions in quantum mechanics
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Students and researchers in quantum mechanics, physicists studying particle exchange phenomena, and anyone interested in the properties of hydrogen isotopes.

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I'm struggling with the relation between particle exchange and parity with the case of para- and ortho-hydrogen.

The overall wavefunction must be antisymmetric with respect to particle exchange and so for para-hydrogen (an antisymmetric spin state) the spatial part of the wavefunction must be symmetric with respect to particle exchange.

My notes say that because the parity of a state of angular momentum quantum number l is (-1)^l then for para-hydrogen l may only take even values. I'm struggling to see the relationship between parity and particle exchange in this case, can anyone help?

Thanks
 
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If \vec{r} is the relative position of the two identical particles, then parity \vec{r} \rightarrow - \vec{r} is formally like particle exchange. Does that make sense? Thus in simple cases the parity of the wavefunction tells you about the symmetry or antisymmetry under particle exchange.

Try it in one dimension to get a feeling for things.

Hope this helps.
 
Yes that makes sense, thank you. If we had a system of say 3 protons the the overall angular momentum would not tell us about the symmetry with respect to particle exchange - is that correct?
 

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