How Is CP-Violation Explored in Particle Physics?

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SUMMARY

This discussion focuses on the exploration of CP-violation in particle physics, specifically addressing the concepts of charge conjugation and parity. Participants highlight the importance of introductory courses in high energy or particle physics, such as those by Perkins, for foundational understanding. The discussion also references Griffith's "Quantum Mechanics" for context, noting that it lacks specific sections on these topics. Additionally, the Wigner theorem is mentioned as a critical concept related to unitary operators and symmetry transformations in Hilbert spaces.

PREREQUISITES
  • Understanding of Quantum Mechanics, particularly Griffith's QM up to Chapter 7
  • Familiarity with concepts of charge conjugation and parity
  • Basic knowledge of high energy/particle physics
  • Awareness of the Wigner theorem and its implications for symmetry in quantum systems
NEXT STEPS
  • Research the electroweak model and its relation to CP-violation
  • Study the Wigner theorem and its application to unitary operators in quantum mechanics
  • Explore introductory courses in high energy physics, such as those by Perkins
  • Investigate the mathematical proof for the operator P^2 and its implications for overall phase in quantum states
USEFUL FOR

This discussion is beneficial for undergraduate physics students, particularly those studying quantum mechanics and interested in advanced topics in particle physics, such as CP-violation and symmetry operations.

Pythagorean
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I've gained interest in the http://lhc.web.cern.ch/lhc/" , which pertain to CP-violation.

QUESTION #1

What sort of classes/branches would teach/contain 'charge conjugation' and 'parity'?

QUESTION #2

the wiki article on parity states that parity is an operator-

"acting on a state ψ as follows: P ψ(r) = ψ(-r). One must have P^2 ψ(r) = e^(i φ) ψ(r), since an overall phase is unobservable."

I'd be interested to see the proof for P^2, and I'm curious how the overall phase being unobservable justifies this (not even sure I know what is meant by the "over all phase")

MY PHYSICS BACKGROUND

I am up to Chapter 7 in Griffith's QM. There doesn't seem to be a section on 'parity' or 'charge conjugation' in the undergrad book, so I am left to wiki
 
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Pythagorean said:
I've gained interest in the http://lhc.web.cern.ch/lhc/" , which pertain to CP-violation.

QUESTION #1

What sort of classes/branches would teach/contain 'charge conjugation' and 'parity'?

QUESTION #2

the wiki article on parity states that parity is an operator-

"acting on a state ψ as follows: P ψ(r) = ψ(-r). One must have P^2 ψ(r) = e^(i φ) ψ(r), since an overall phase is unobservable."

I'd be interested to see the proof for P^2, and I'm curious how the overall phase being unobservable justifies this (not even sure I know what is meant by the "over all phase")

MY PHYSICS BACKGROUND

I am up to Chapter 7 in Griffith's QM. There doesn't seem to be a section on 'parity' or 'charge conjugation' in the undergrad book, so I am left to wiki

Q1) See QFT Dirac field,KG charged field etc... electroweak model...
Q2)See wigner theorem... its on unitary operator acting on hilbert spaces that implement a symmetry trasf..


regards
 
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Pythagorean said:
QUESTION #1

What sort of classes/branches would teach/contain 'charge conjugation' and 'parity'?

An intro course in high energy/particle physics at the level of Perkins would give you a first glimpse of such a thing.

Zz.
 

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