Fixing CP phases to cancel CKM phases

In summary, when trying to determine if the weak sector is CP invariant, we CP transform all the fields in the charged interaction terms and obtain a condition involving the elements of the CKM matrix and the arbitrary phases of the CP transformed fields. This condition requires fixing the CP phases to cancel the 6 CKM phases, but there are only 5 independent CP phases due to the presence of 2 residual global symmetries (U(1)B and U(1)Q) corresponding to baryon number and electric charge. This means that there is always 1 phase remaining in the CKM matrix that cannot be canceled, making the condition impossible to hold.
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Siupa
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When we try to see if the weak sector is CP invariant, we CP transform all the fields in the charged interactions terms and we get a condition involving the elements of the CKM matrix and the arbitrary phases of the CP transformed fields:
$$V_{ij} = V^*_{ij} \, e^{i(\xi_W + \phi_{d_j} - \phi_{u_i})}$$
Then, the argument goes: there are 9 parameters in V_CKM because it is a general 3x3 unitary matrix. These 9 parameters are split in 3 "angles" and 6 phases, the 3 angles being the ones you get if you restrict to an element of ##\text{SO}(3)##.

To make the above condition hold, we need to fix the CP phases to cancel the 6 CKM phases. We have 7 CP phases (1 from W, 3 from the downs and 3 from the ups), so it seems like we can do it.

But then we say "actually we have only 5 independent CP phases, because there are 2 residual global symmetries corresponding to baryon number and electric charge". Therefore, 1 phase remains in the CKM and the condition can never hold.

I don't understand the last point: why does the presence of ##\text{U}(1)_\text{B}## and ##\text{U}(1)_\text{Q}## global symmetries reduces the number of CP phases I can fix to cancel the CKM phases?
 
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You can use two of those phases to be included in your U(1)B and U(1)Q global transformations of your fields (one for each transformation)
 
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1. What is CP violation and why is it important?

CP violation refers to the violation of the combined symmetry of charge conjugation (C) and parity (P) in particle physics. It is important because it helps explain the observed dominance of matter over antimatter in the universe.

2. What is CKM matrix and how does it relate to CP violation?

The Cabibbo-Kobayashi-Maskawa (CKM) matrix is a unitary matrix that describes the mixing of quark flavors in the weak interaction. It relates to CP violation because the non-zero off-diagonal elements in the CKM matrix allow for the possibility of CP violation in the weak interaction.

3. How does fixing CP phases cancel CKM phases?

Fixing CP phases refers to choosing a specific phase convention for the CKM matrix. This convention cancels out the phases in the CKM matrix, making it real and eliminating the possibility of CP violation in the weak interaction.

4. Are there any experimental evidence for fixing CP phases?

Yes, there is experimental evidence for fixing CP phases. Measurements of CP violation in the quark sector have been consistent with the Standard Model predictions, which assumes fixed CP phases.

5. What are the implications of fixing CP phases for future research?

Fixing CP phases has important implications for future research in particle physics. It allows for a simpler and more precise description of CP violation, making it easier to test for new physics beyond the Standard Model. It also helps to reduce theoretical uncertainties in calculations and predictions.

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