Psi Meson Decay Modes: Spin, Parity, Quark Content & More

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SUMMARY

The discussion focuses on the decay modes of the Psi meson, specifically the J/psi particle, detailing its spin, parity, and quark content. The spin of mesons can be either 0 or 1, with parity calculated using the formula ##(-1)^{L+1}##. The quark content for J/psi is identified as charm and anti-charm (##c\bar c##). The discussion also addresses the reasons for the decay patterns, including the kinematic constraints that prevent certain decay modes and the minimum center of mass energy required for decay processes involving the ##\chi## states.

PREREQUISITES
  • Understanding of quantum mechanics and particle physics
  • Familiarity with meson classification and properties
  • Knowledge of Feynman diagrams and decay processes
  • Basic grasp of strong and weak interactions in particle physics
NEXT STEPS
  • Research the properties of other mesons, such as the B meson and its decay modes
  • Study the implications of spin and parity in particle interactions
  • Learn about the role of Feynman diagrams in predicting particle decay outcomes
  • Explore the differences between strong and weak interactions in particle physics
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Particle physicists, students studying quantum mechanics, and researchers interested in meson decay processes and their implications in high-energy physics.

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Homework Statement



(a) Explain spin and parity of mesons
(b) State their quark content
(c) Draw a feynman diagram of J/psi decay
(d) Why doesn't ##\chi## undergo leptonic decay?
(e) What is the minimum centre of mass? [/B]

2013_B4_Q1.png

Homework Equations

The Attempt at a Solution



Part(a)[/B]
Spin is either 0 (singlet) or 1 (tripplet) for a pair of fermions. Parity is given by ##(-1)^{L+1}##.

Part(b)
Quark content is charm and anti-charm hadron ##c\bar c##. For ##1^-## states, ##L=0, S=1, J=1##. For ##0^+## states, ##L=1, S=1, J=0## through spin-orbit coupling. For ##1^+## states, ##L=1, S=0, J=1##. For ##2^+## states, ##L=S=1, J=2##.

Part(c)
EM decay of J\Psi to either ##e^+e^-## or ##\mu^+ \mu^-##:
2013_B4_Q1_2.png


Part (d)
Previously, it was kinematically impossible for strong interactions. Now that the mass of excited ##\psi^{''}## is higher, there is a direct possibility of decay in strong interaction to ##D^+D^-##. Strong interactions are preferred over weak interactions.

Part (e)
Why doesn't ##\chi## decay to pairs of charged leptons?
Possible reaction for ##\psi^{'} \rightarrow \chi_0 + \mu^{+} + \mu^{-}## or ##\psi^{'} \rightarrow \chi_0 + e^{+} + e^{-}##
2013_B4_Q1_3.png

For decay to ##\chi_1## and ##\chi_2## only ##e^{-}e^{+}## pairs are allowed.

Part (f)
I suppose minimum mass is ##m_{\chi2} + 2m_e = 3557 MeV##.
What are the important elements?
 
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bumpp
 
Important elements?
 
What are the important elements in a detector?
 
bumpppppp
 
what things that are important make a reactor?
 
For part (f) : Isn't the minimum centre of mass energy for ##\chi## decays to be observed simply the mass of ##m_\chi = 3415 MeV/c^2##?
 
bumpp part (f)
 
bump on part (f) Centre of mass energy?
 
  • #10
bumpp on part (f)
 
  • #11
bump on (f): Centre of Mass Energy
 
  • #12
bumpp - Centre of mass energy?
 
  • #13
bumpp on part (f)
 
  • #14
bumpp - is my centre of mass energy right? Part (f)
 

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