G-parity - where does the minus sign come from?

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SUMMARY

The discussion centers on the concept of G-parity in particle physics, specifically its mathematical definition as G = exp(-iπ Iy)C, where Iy represents the second component of isospin and C denotes C-parity. Participants explore the application of G-parity to the isospin doublet (u, d), resulting in the transformation to - (d̅, u̅). The minus sign arises from the properties of the G-parity operator and the requirement that the doublet must be in an eigenstate of G, which is not satisfied in the given context.

PREREQUISITES
  • Understanding of isospin and its components
  • Familiarity with C-parity and its implications
  • Knowledge of quantum mechanics, specifically operator theory
  • Basic grasp of particle physics terminology
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  • Study the mathematical properties of G-parity in quantum field theory
  • Research the implications of isospin transformations on particle states
  • Learn about eigenstates and eigenvalues in quantum mechanics
  • Explore the role of symmetry operations in particle physics
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Particle physicists, quantum mechanics students, and researchers interested in the symmetries of particle interactions and transformations.

Federica
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Hi all,

I have a question on G-parity. I know it's defined as ## G = exp(-i\pi I_{y})C ##, with ##I_y## being the second component of the isospin and ##C## is the C-parity. In other words, the G-parity should be the C-parity followed by a 180° rotation around the second axis of the isospin.

Now, if I apply C on the isospin doublet ## \begin{pmatrix} u\\ d \end{pmatrix} ## I get ## \begin{pmatrix} \bar{u}\\ \bar{d} \end{pmatrix} ##, which is quite clear.

If I apply the G-parity on the same doublet I get: ## -\begin{pmatrix} \bar{d}\\ \bar{u} \end{pmatrix} ##. I understand ##\bar{d}## and ##\bar{u}## are now inverted because of the rotation around ##I_y##, but where does the minus sign come from?
 
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Federica said:
but where does the minus sign come from?

The definition.

I am not sure what kind of answer would satisfy you. Why isn't "the definition" a good answer?
 
Vanadium 50 said:
The definition.

I am not sure what kind of answer would satisfy you. Why isn't "the definition" a good answer?
I understand why the third component of the isospin changes its sign, that's because of the rotation. But why should I put a minus sign in front of the whole doublet?
 
Sorry, I was confused about which minus sign you meant.

You are not in an eigenstate of G with the doublet you wrote. So -1 can't be the eigenvalue because there isn't an eigenvalue.
 

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