How Is CP-Violation Explored in Particle Physics?

  • Thread starter Thread starter Pythagorean
  • Start date Start date
  • Tags Tags
    Parity
Click For Summary
CP-violation in particle physics is explored through concepts like charge conjugation and parity, which are foundational in understanding symmetries in quantum mechanics. Relevant classes include introductory courses in high energy or particle physics, such as those based on Perkins' texts, as well as more advanced topics in quantum field theory. The discussion highlights the operator nature of parity, with specific interest in the proof of P^2 and the implications of an unobservable overall phase. The Wigner theorem is referenced as a key resource for understanding symmetry transformations in Hilbert spaces. Overall, a solid grasp of these concepts is essential for delving into CP-violation studies.
Pythagorean
Science Advisor
Messages
4,416
Reaction score
327
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
 
Last edited by a moderator:
Physics news on Phys.org
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
 
Last edited by a moderator:
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.
 
Insights auto threads is broken atm, so I'm manually creating these for new Insight articles. Towards the end of the first lecture for the Qiskit Global Summer School 2025, Foundations of Quantum Mechanics, Olivia Lanes (Global Lead, Content and Education IBM) stated... Source: https://www.physicsforums.com/insights/quantum-entanglement-is-a-kinematic-fact-not-a-dynamical-effect/ by @RUTA

Similar threads

  • · Replies 7 ·
Replies
7
Views
2K
  • · Replies 9 ·
Replies
9
Views
2K
  • · Replies 16 ·
Replies
16
Views
3K
Replies
7
Views
2K
  • · Replies 4 ·
Replies
4
Views
2K
Replies
1
Views
1K
  • · Replies 2 ·
Replies
2
Views
4K
  • · Replies 15 ·
Replies
15
Views
2K
Replies
1
Views
2K
Replies
7
Views
5K